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Hindawi Publishing CorporationThe Scientific World JournalVolume 2013 Article ID 187452 12 pageshttpdxdoiorg1011552013187452
Research ArticleOn a Family of Multivariate Modified Humbert Polynomials
Rabia AktaG1 and Esra ErkuG-Duman2
1 Department of Mathematics Faculty of Science Ankara University Tandogan 06100 Ankara Turkey2Department of Mathematics Faculty of Science Gazi University Teknikokullar 06500 Ankara Turkey
Correspondence should be addressed to Rabia Aktas raktasscienceankaraedutr
Received 29 April 2013 Accepted 6 June 2013
Academic Editors F J Garcia-Pacheco and V Privman
Copyright copy 2013 R Aktas and E Erkus-Duman This is an open access article distributed under the Creative CommonsAttribution License which permits unrestricted use distribution and reproduction in any medium provided the original work isproperly cited
This paper attempts to present a multivariable extension of generalized Humbert polynomials The results obtained here includevarious families ofmultilinear andmultilateral generating functions miscellaneous properties and also some special cases for thesemultivariable polynomials
1 Introduction
The generalized Humbert polynomials are generated by [1]
(119862 minus 119898119909119905 + 119910119905119898)119901
=infin
sum119899=0
119875119899(119898 119909 119910 119901 119862) 119905119899 (1)
where 119898 is a positive integer and other parameters areunrestricted in general (see also [2 pages 77 86] and [34]) This definition includes many well-known special poly-nomials such as Humbert Louville Gegenbauer LegendreTchebycheff Pincherle and Kinney polynomials
In this paper we consider the following multivariableextension of the generalized Humbert polynomials which arecompletely different from the polynomials introduced in [5]This class of polynomials is generated by
(1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(1003816100381610038161003816100381610038161003816100381610038161003816
119903
sum119894=1
(119898119894119909119894t119894minus 119910
119894119905119898119894119894)1003816100381610038161003816100381610038161003816100381610038161003816lt 1)
(2)
where x = (1199091 119909
119903) y = (119910
1 119910
119903)m = (119898
1 119898
119903)
and 119898119894(119894 = 1 2 119903) is a positive integer It follows from
(2) that
Θ(120572)
1198991 119899119903
(x ym)
=[11989911198981]
sum1198961=0
sdot sdot sdot[119899119903119898119903]
sum119896119903=0
(120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
1198961 sdot sdot sdot 119896
119903 (119899
1minus 119898
11198961) sdot sdot sdot (119899
119903minus 119898
119903119896119903)
times (minus1)1198961+sdotsdotsdot+119896119903(11989811199091)1198991minus11989811198961 sdot sdot sdot (119898
119903119909119903)119899119903minus1198981199031198961199031199101198961
1sdot sdot sdot 119910119896119903
119903
(3)
where (120582)119896
= 120582(120582 + 1) sdot sdot sdot (120582 + 119896 minus 1) (120582)0= 1 is the
Pochhammer symbolThe aim of this paper is to derive various families of
multilinear and multilateral generating functions and to giveseveral recurrence relations and expansions in the seriesof orthogonal polynomials for the family of multivariablepolynomials given explicitly by (3) We present some specialcases of our results and also obtain some other properties forthese special cases
2 Bilinear and Bilateral Generating Functions
In this section with the help of the similar method asconsidered in [5ndash9] we derive several families of bilinear and
2 The Scientific World Journal
bilateral generating functions for the family of multivariablepolynomials generated by (2) and given explicitly by (3)
We begin by stating the following theorem
Theorem 1 Corresponding to an identically nonvanishingfunction Ω
120583(z) of 119904 complex variables 119911
1 119911
119904(119904 isin N) and
of complex order 120583 let
Λ120583] (z 119908) =
infin
sum119896=0
119886119896Ω120583+]119896 (z) 119908
119896 (4)
where (119886119896
= 0 120583 ] isin C) z = (1199111 119911
119904)Then for119901 isin N x =
(1199091 119909
119903) y = (y
1 yr) m = (119898
1 119898
119903) 119898
119894isin N (119894 =
1 2 119903) one has
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
119886119896Θ(120572)
1198991minus1199011198961198992119899119903
(x ym)
times 11990511989922sdot sdot sdot 119905119899119903
119903Ω120583+]119896 (z) 120578
1198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(5)
provided that each member of (5) exists
Proof For convenience let 119878 denote the first member of theassertion (5) of Theorem 1 Replacing 119899
1by 119899
1+ 119901119896 we may
write that
119878 =infin
sum1198991 119899119903=0
infin
sum119896=0
119886119896Θ(120572)
11989911198992 119899119903
(x ym)Ω120583+]119896 (z) 120578
11989611990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 1198992119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
infin
sum119896=0
119886119896Ω120583+]119896 (z) 120578
119896
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(6)
which completes the proof
By using a similar idea we also get the next result imme-diately
Theorem 2 For a nonvanishing function 1205931205821 120582119903
(z) of 119904complex variables 119911
1 119911
119904(119904 isin N) and for 119901
119894isin N 120582
119894 120578
119894isin C
z = (1199111 119911
119904) w = (119908
1 119908
119903) 120582 = (120582
1 120582
119903) 120578 =
(1205781 120578
119903) let
Ωnp120582120578120572120573m (x y zw)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(x ym)
times 1205931205821+12057811198961 120582119903+120578119903119896119903
(z) 1199081198961
1sdot sdot sdot 119908119896119903
119903(7)
where 1198861198961 119896119903
= 0 119899119894 (119894 = 1 2 119903) isin N
0 N
0= N cup 0
Then one has
1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572)
1198991minus1198971 119899119903minus119897119903
(x ym)
times Θ(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(x ym)
times 1205931205821+12057811198961 120582r+120578119903119896119903
(z)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ωnp120582120578120572120573m (x y zw)
(8)
provided that each member of (8) exists
3 Special Cases
As an application of the above theorems when the multi-variable function Ω
120583+]119896(z) z = (1199111 119911
119904) 119896 isin N
0 119904 isin N
is expressed in terms of simpler functions of one and morevariables then we can give further applications of the abovetheorems We first set
119904 = 119903 Ω120583+]119896 (z) = g(1205731 120573119903)
120583+]119896 (z) (9)
in Theorem 1 where the Chan-Chyan-Srivastava polynomi-als g(1205731 120573119903)
120583+]119896 (z) [10] are generated by
119903
prod119894=1
(1 minus 119909119894119905)minus120572119894 =
infin
sum119899=0
g(1205721120572119903)119899
(1199091 119909
119903) 119905119899
(120572119894isin C (119894 = 1 2 119903) |119905| lt min 10038161003816100381610038161199091
1003816100381610038161003816minus1
10038161003816100381610038161199091199031003816100381610038161003816minus1
) (10)
We are thus led to the following result which provides aclass of bilateral generating functions for the Chan-Chyan-Srivastava polynomials and the family of multivariable poly-nomials given explicitly by (3)
Corollary 3 If Λ120583](z 119908) = suminfin
119896=0119886119896g (1205731 120573119903)
120583+]119896 (z)119908119896 119886119896
= 0120583 ] isin C z = (119911
1 119911
119903) then one has
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
119886119896Θ(120572)
1198991minus1199011198961198992 119899119903
(x ym)
times 11990511989922sdot sdot sdot 119905119899119903
119903g (1205731 120573119903)
120583+]119896 (z) 1205781198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(11)
provided that each member of (11) exists
The Scientific World Journal 3
Remark 4 Using the generating relation (10) for the Chan-Chyan-Srivastava polynomials and getting 119886
119896= 1 120583 = 0 ] =
1 we find that
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
Θ(120572)
1198991minus1199011198961198992 119899119903
(x ym) 11990511989922sdot sdot sdot 119905119899119903
119903g(1205731 120573119903)119896
(z)
times 1205781198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572119903
prod119894=1
(1 minus 119911119894120578)
minus120573119894
10038161003816100381610038161205781003816100381610038161003816 lt min 10038161003816100381610038161199111
1003816100381610038161003816minus1
10038161003816100381610038161199111199031003816100381610038161003816minus1
1003816100381610038161003816100381610038161003816100381610038161003816
119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894)1003816100381610038161003816100381610038161003816100381610038161003816lt 1
(12)
On the other hand choosing 119904 = 2119903 and
1205931205821+12057811198961 120582119903+120578119903119896119903
(z) = Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) (13)
120582119894 120578
119894(119894 = 1 2 119903) isin N
0 u = (119906
1 119906
119903) k = (V
1
V119903) inTheorem 2 we obtain the following class of bilinear
generating functions for the family of multivariable polyno-mials given explicitly by (3)
Corollary 5 If
Λnp120582120578120572120573120574m (x y u kw)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(x ym)
times Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) 1199081198961
1sdot sdot sdot 119908119896119903
119903
(14)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 then
we get
1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572)
1198991minus1198971 119899119903minus119897119903
(x ym)
times Θ(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(x ym)
timesΘ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Λnp120582120578120572120573120574m (x y u kw)
(15)
provided that each member of (15) exists
Furthermore for every suitable choice of the coefficients119886119896
(119896 isin N0) if the multivariable functions Ω
120583+]119896(y) and1205931205821+12057811198961 120582119903+120578119903119896119903
(y) y = (1199101 119910
119904) (119904 isin N) are expressed
as an appropriate product of several simpler functions theassertions of Theorems 1 and 2 can be applied in orderto derive various families of multilinear and multilateral
generating functions for the family of multivariable polyno-mials given explicitly by (3)
4 Some Miscellaneous Properties
In this section we now discuss some further properties ofthe family of multivariable polynomials given by (3)We startwith the following theorems
Theorem 6 Let Ψ1198991119899119903
(x ym) be a family of functionsgenerated by
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
=infin
sum1198991 119899119903=0
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(16)
The following relations hold
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(17)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym) (18)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also one
finds that
119898119894119909119894
120597
120597119910119894
Ψ1198991119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Ψ
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903(x ym)
(19)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119903
(x ym) = 0 (20)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
4 The Scientific World Journal
Proof Fix 119894 = 1 2 119903 Then by differentiating (16) withrespect to 119909
119894and 119905
119894 after making necessary calculations we
obtain thatinfin
sum1198991119899119903=0
119899119894Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (119909119894minus 119910
119894119905119898119894minus1119894
)infin
sum1198991119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119909119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
minus 119910119894
infin
sum1198991 119899119894minus1119899119894+1119899119903=0
(119899119894ge119898119894minus1)
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
times 11990511989911sdot sdot sdot 119905119899119903
119903
(21)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain (17) and
(18) for the fixed 119894 Similarly if we differentiate (16) withrespect to 119910
119894and 119905
119894 we can find the relation (19)
Theorem 7 If Ψ1198991119899119903
(x ym) is a family of functions gener-ated by (16) then it satisfies the relations
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(22)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (23)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Proof By comparing the derivatives of (16) with respect to 119909119894
and 119910119894 we have
minus 119898119894119905119894
infin
sum1198991 119899119903=0
120597
120597119910119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119905119898119894119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(24)
which implies that
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(25)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (26)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Thus
the proof is completed
As a result of these theorems if we choose
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
(27)
then we can give some recurrence relations for the family ofmultivariable polynomials given explicitly by (3) In the viewof Theorem 6 we get
Corollary 8 For the family of multivariable polynomialsgenerated by (2) the following relations hold
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
(28)
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Θ(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(29)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also for 119899
119894=
0 1 119898119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 we have
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym) (30)
120597
120597119910119894
Θ(120572)
1198991119899119903
(x ym) = 0 (31)
Corollary 9 By summing the relations given by (28) and (29)respectively for 119894 = 1 2 119903 we get
119903
sum119894=1
119899119894Θ(120572)
1198991119899119903
(x ym)
=119903
sum119894=1
119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus119903
sum119894=1
119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
The Scientific World Journal 5
119903
sum119894=1
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym)
minus119903
sum119894=1
119898119894119910119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
= minus119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(32)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Similarly as a consequence ofTheorem 7 we can give thenext result at once
Corollary 10 Other recurrence relations for the family ofmultivariable polynomials Θ(120572)
1198991119899119903
(x ym) are
minus 119898119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(33)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (34)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Theorem 11 The generating relation (2) yields the followingaddition formula for the family of multivariable polynomialsgiven by (3)
Θ(120572+120573)
1198991119899119903
(x ym) =1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym)
(35)
Proof From (2) we have
infin
sum1198991 119899119903=0
Θ(120572+120573)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus(120572+120573)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
times (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120573
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
timesinfin
sum1198961 119896119903=0
Θ(120573)
1198961 119896119903
(x ym) 11990511989611sdot sdot sdot 119905119896119903
119903
(36)
Replacing 119899119894by 119899
119894minus 119896
119894 119894 = 1 2 119903 the right-hand side of
the last equality is
infin
sum1198991119899119903=0
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(37)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903completes the proof
We now give expansions of the family of multivariablepolynomialsΘ(120572)
1198991119899119903
(x ym) given explicitly by (3) in series ofLegendre Gegenbauer Hermite and Laguerre polynomials
Theorem 12 Expansions of Θ(120572)
1198991119899119903
(x ym) in series of Leg-endre Gegenbauer Hermite and Laguerre polynomials are asfollows
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus119898119894119896119894minus119904119894
times(minus1)119896119894119910119896119894119894119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 119898
119894119896119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus119898119894119896119894minus119904119894+1
times(minus119910119894)119896119894119862]119894
119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898i]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(minus119910119894)119896119894119867
119899119894minus119898119894119896119894minus2119904119894(119898
1198941199091198942)
119896119894119904119894 (119899
119894minus 119898
119894119896119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
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International Journal of Mathematics and Mathematical Sciences
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The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
2 The Scientific World Journal
bilateral generating functions for the family of multivariablepolynomials generated by (2) and given explicitly by (3)
We begin by stating the following theorem
Theorem 1 Corresponding to an identically nonvanishingfunction Ω
120583(z) of 119904 complex variables 119911
1 119911
119904(119904 isin N) and
of complex order 120583 let
Λ120583] (z 119908) =
infin
sum119896=0
119886119896Ω120583+]119896 (z) 119908
119896 (4)
where (119886119896
= 0 120583 ] isin C) z = (1199111 119911
119904)Then for119901 isin N x =
(1199091 119909
119903) y = (y
1 yr) m = (119898
1 119898
119903) 119898
119894isin N (119894 =
1 2 119903) one has
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
119886119896Θ(120572)
1198991minus1199011198961198992119899119903
(x ym)
times 11990511989922sdot sdot sdot 119905119899119903
119903Ω120583+]119896 (z) 120578
1198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(5)
provided that each member of (5) exists
Proof For convenience let 119878 denote the first member of theassertion (5) of Theorem 1 Replacing 119899
1by 119899
1+ 119901119896 we may
write that
119878 =infin
sum1198991 119899119903=0
infin
sum119896=0
119886119896Θ(120572)
11989911198992 119899119903
(x ym)Ω120583+]119896 (z) 120578
11989611990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 1198992119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
infin
sum119896=0
119886119896Ω120583+]119896 (z) 120578
119896
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(6)
which completes the proof
By using a similar idea we also get the next result imme-diately
Theorem 2 For a nonvanishing function 1205931205821 120582119903
(z) of 119904complex variables 119911
1 119911
119904(119904 isin N) and for 119901
119894isin N 120582
119894 120578
119894isin C
z = (1199111 119911
119904) w = (119908
1 119908
119903) 120582 = (120582
1 120582
119903) 120578 =
(1205781 120578
119903) let
Ωnp120582120578120572120573m (x y zw)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(x ym)
times 1205931205821+12057811198961 120582119903+120578119903119896119903
(z) 1199081198961
1sdot sdot sdot 119908119896119903
119903(7)
where 1198861198961 119896119903
= 0 119899119894 (119894 = 1 2 119903) isin N
0 N
0= N cup 0
Then one has
1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572)
1198991minus1198971 119899119903minus119897119903
(x ym)
times Θ(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(x ym)
times 1205931205821+12057811198961 120582r+120578119903119896119903
(z)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ωnp120582120578120572120573m (x y zw)
(8)
provided that each member of (8) exists
3 Special Cases
As an application of the above theorems when the multi-variable function Ω
120583+]119896(z) z = (1199111 119911
119904) 119896 isin N
0 119904 isin N
is expressed in terms of simpler functions of one and morevariables then we can give further applications of the abovetheorems We first set
119904 = 119903 Ω120583+]119896 (z) = g(1205731 120573119903)
120583+]119896 (z) (9)
in Theorem 1 where the Chan-Chyan-Srivastava polynomi-als g(1205731 120573119903)
120583+]119896 (z) [10] are generated by
119903
prod119894=1
(1 minus 119909119894119905)minus120572119894 =
infin
sum119899=0
g(1205721120572119903)119899
(1199091 119909
119903) 119905119899
(120572119894isin C (119894 = 1 2 119903) |119905| lt min 10038161003816100381610038161199091
1003816100381610038161003816minus1
10038161003816100381610038161199091199031003816100381610038161003816minus1
) (10)
We are thus led to the following result which provides aclass of bilateral generating functions for the Chan-Chyan-Srivastava polynomials and the family of multivariable poly-nomials given explicitly by (3)
Corollary 3 If Λ120583](z 119908) = suminfin
119896=0119886119896g (1205731 120573119903)
120583+]119896 (z)119908119896 119886119896
= 0120583 ] isin C z = (119911
1 119911
119903) then one has
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
119886119896Θ(120572)
1198991minus1199011198961198992 119899119903
(x ym)
times 11990511989922sdot sdot sdot 119905119899119903
119903g (1205731 120573119903)
120583+]119896 (z) 1205781198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
Λ120583] (z 120578)
(11)
provided that each member of (11) exists
The Scientific World Journal 3
Remark 4 Using the generating relation (10) for the Chan-Chyan-Srivastava polynomials and getting 119886
119896= 1 120583 = 0 ] =
1 we find that
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
Θ(120572)
1198991minus1199011198961198992 119899119903
(x ym) 11990511989922sdot sdot sdot 119905119899119903
119903g(1205731 120573119903)119896
(z)
times 1205781198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572119903
prod119894=1
(1 minus 119911119894120578)
minus120573119894
10038161003816100381610038161205781003816100381610038161003816 lt min 10038161003816100381610038161199111
1003816100381610038161003816minus1
10038161003816100381610038161199111199031003816100381610038161003816minus1
1003816100381610038161003816100381610038161003816100381610038161003816
119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894)1003816100381610038161003816100381610038161003816100381610038161003816lt 1
(12)
On the other hand choosing 119904 = 2119903 and
1205931205821+12057811198961 120582119903+120578119903119896119903
(z) = Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) (13)
120582119894 120578
119894(119894 = 1 2 119903) isin N
0 u = (119906
1 119906
119903) k = (V
1
V119903) inTheorem 2 we obtain the following class of bilinear
generating functions for the family of multivariable polyno-mials given explicitly by (3)
Corollary 5 If
Λnp120582120578120572120573120574m (x y u kw)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(x ym)
times Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) 1199081198961
1sdot sdot sdot 119908119896119903
119903
(14)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 then
we get
1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572)
1198991minus1198971 119899119903minus119897119903
(x ym)
times Θ(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(x ym)
timesΘ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Λnp120582120578120572120573120574m (x y u kw)
(15)
provided that each member of (15) exists
Furthermore for every suitable choice of the coefficients119886119896
(119896 isin N0) if the multivariable functions Ω
120583+]119896(y) and1205931205821+12057811198961 120582119903+120578119903119896119903
(y) y = (1199101 119910
119904) (119904 isin N) are expressed
as an appropriate product of several simpler functions theassertions of Theorems 1 and 2 can be applied in orderto derive various families of multilinear and multilateral
generating functions for the family of multivariable polyno-mials given explicitly by (3)
4 Some Miscellaneous Properties
In this section we now discuss some further properties ofthe family of multivariable polynomials given by (3)We startwith the following theorems
Theorem 6 Let Ψ1198991119899119903
(x ym) be a family of functionsgenerated by
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
=infin
sum1198991 119899119903=0
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(16)
The following relations hold
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(17)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym) (18)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also one
finds that
119898119894119909119894
120597
120597119910119894
Ψ1198991119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Ψ
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903(x ym)
(19)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119903
(x ym) = 0 (20)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
4 The Scientific World Journal
Proof Fix 119894 = 1 2 119903 Then by differentiating (16) withrespect to 119909
119894and 119905
119894 after making necessary calculations we
obtain thatinfin
sum1198991119899119903=0
119899119894Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (119909119894minus 119910
119894119905119898119894minus1119894
)infin
sum1198991119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119909119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
minus 119910119894
infin
sum1198991 119899119894minus1119899119894+1119899119903=0
(119899119894ge119898119894minus1)
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
times 11990511989911sdot sdot sdot 119905119899119903
119903
(21)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain (17) and
(18) for the fixed 119894 Similarly if we differentiate (16) withrespect to 119910
119894and 119905
119894 we can find the relation (19)
Theorem 7 If Ψ1198991119899119903
(x ym) is a family of functions gener-ated by (16) then it satisfies the relations
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(22)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (23)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Proof By comparing the derivatives of (16) with respect to 119909119894
and 119910119894 we have
minus 119898119894119905119894
infin
sum1198991 119899119903=0
120597
120597119910119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119905119898119894119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(24)
which implies that
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(25)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (26)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Thus
the proof is completed
As a result of these theorems if we choose
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
(27)
then we can give some recurrence relations for the family ofmultivariable polynomials given explicitly by (3) In the viewof Theorem 6 we get
Corollary 8 For the family of multivariable polynomialsgenerated by (2) the following relations hold
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
(28)
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Θ(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(29)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also for 119899
119894=
0 1 119898119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 we have
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym) (30)
120597
120597119910119894
Θ(120572)
1198991119899119903
(x ym) = 0 (31)
Corollary 9 By summing the relations given by (28) and (29)respectively for 119894 = 1 2 119903 we get
119903
sum119894=1
119899119894Θ(120572)
1198991119899119903
(x ym)
=119903
sum119894=1
119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus119903
sum119894=1
119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
The Scientific World Journal 5
119903
sum119894=1
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym)
minus119903
sum119894=1
119898119894119910119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
= minus119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(32)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Similarly as a consequence ofTheorem 7 we can give thenext result at once
Corollary 10 Other recurrence relations for the family ofmultivariable polynomials Θ(120572)
1198991119899119903
(x ym) are
minus 119898119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(33)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (34)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Theorem 11 The generating relation (2) yields the followingaddition formula for the family of multivariable polynomialsgiven by (3)
Θ(120572+120573)
1198991119899119903
(x ym) =1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym)
(35)
Proof From (2) we have
infin
sum1198991 119899119903=0
Θ(120572+120573)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus(120572+120573)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
times (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120573
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
timesinfin
sum1198961 119896119903=0
Θ(120573)
1198961 119896119903
(x ym) 11990511989611sdot sdot sdot 119905119896119903
119903
(36)
Replacing 119899119894by 119899
119894minus 119896
119894 119894 = 1 2 119903 the right-hand side of
the last equality is
infin
sum1198991119899119903=0
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(37)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903completes the proof
We now give expansions of the family of multivariablepolynomialsΘ(120572)
1198991119899119903
(x ym) given explicitly by (3) in series ofLegendre Gegenbauer Hermite and Laguerre polynomials
Theorem 12 Expansions of Θ(120572)
1198991119899119903
(x ym) in series of Leg-endre Gegenbauer Hermite and Laguerre polynomials are asfollows
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus119898119894119896119894minus119904119894
times(minus1)119896119894119910119896119894119894119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 119898
119894119896119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus119898119894119896119894minus119904119894+1
times(minus119910119894)119896119894119862]119894
119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898i]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(minus119910119894)119896119894119867
119899119894minus119898119894119896119894minus2119904119894(119898
1198941199091198942)
119896119894119904119894 (119899
119894minus 119898
119894119896119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
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Discrete Dynamics in Nature and Society
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
The Scientific World Journal 3
Remark 4 Using the generating relation (10) for the Chan-Chyan-Srivastava polynomials and getting 119886
119896= 1 120583 = 0 ] =
1 we find that
infin
sum1198991 119899119903=0
[1198991119901]
sum119896=0
Θ(120572)
1198991minus1199011198961198992 119899119903
(x ym) 11990511989922sdot sdot sdot 119905119899119903
119903g(1205731 120573119903)119896
(z)
times 1205781198961199051198991minus1199011198961
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572119903
prod119894=1
(1 minus 119911119894120578)
minus120573119894
10038161003816100381610038161205781003816100381610038161003816 lt min 10038161003816100381610038161199111
1003816100381610038161003816minus1
10038161003816100381610038161199111199031003816100381610038161003816minus1
1003816100381610038161003816100381610038161003816100381610038161003816
119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894)1003816100381610038161003816100381610038161003816100381610038161003816lt 1
(12)
On the other hand choosing 119904 = 2119903 and
1205931205821+12057811198961 120582119903+120578119903119896119903
(z) = Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) (13)
120582119894 120578
119894(119894 = 1 2 119903) isin N
0 u = (119906
1 119906
119903) k = (V
1
V119903) inTheorem 2 we obtain the following class of bilinear
generating functions for the family of multivariable polyno-mials given explicitly by (3)
Corollary 5 If
Λnp120582120578120572120573120574m (x y u kw)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(x ym)
times Θ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km) 1199081198961
1sdot sdot sdot 119908119896119903
119903
(14)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 then
we get
1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
Θ(120572)
1198991minus1198971 119899119903minus119897119903
(x ym)
times Θ(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(x ym)
timesΘ(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(u km)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Λnp120582120578120572120573120574m (x y u kw)
(15)
provided that each member of (15) exists
Furthermore for every suitable choice of the coefficients119886119896
(119896 isin N0) if the multivariable functions Ω
120583+]119896(y) and1205931205821+12057811198961 120582119903+120578119903119896119903
(y) y = (1199101 119910
119904) (119904 isin N) are expressed
as an appropriate product of several simpler functions theassertions of Theorems 1 and 2 can be applied in orderto derive various families of multilinear and multilateral
generating functions for the family of multivariable polyno-mials given explicitly by (3)
4 Some Miscellaneous Properties
In this section we now discuss some further properties ofthe family of multivariable polynomials given by (3)We startwith the following theorems
Theorem 6 Let Ψ1198991119899119903
(x ym) be a family of functionsgenerated by
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
=infin
sum1198991 119899119903=0
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(16)
The following relations hold
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(17)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
119899119894Ψ1198991119899119903
(x ym) = 119909119894
120597
120597119909119894
Ψ1198991119899119903
(x ym) (18)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also one
finds that
119898119894119909119894
120597
120597119910119894
Ψ1198991119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Ψ
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903(x ym)
(19)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119903
(x ym) = 0 (20)
for 119899119894= 0 1 119898
119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
4 The Scientific World Journal
Proof Fix 119894 = 1 2 119903 Then by differentiating (16) withrespect to 119909
119894and 119905
119894 after making necessary calculations we
obtain thatinfin
sum1198991119899119903=0
119899119894Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (119909119894minus 119910
119894119905119898119894minus1119894
)infin
sum1198991119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119909119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
minus 119910119894
infin
sum1198991 119899119894minus1119899119894+1119899119903=0
(119899119894ge119898119894minus1)
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
times 11990511989911sdot sdot sdot 119905119899119903
119903
(21)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain (17) and
(18) for the fixed 119894 Similarly if we differentiate (16) withrespect to 119910
119894and 119905
119894 we can find the relation (19)
Theorem 7 If Ψ1198991119899119903
(x ym) is a family of functions gener-ated by (16) then it satisfies the relations
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(22)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (23)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Proof By comparing the derivatives of (16) with respect to 119909119894
and 119910119894 we have
minus 119898119894119905119894
infin
sum1198991 119899119903=0
120597
120597119910119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119905119898119894119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(24)
which implies that
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(25)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (26)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Thus
the proof is completed
As a result of these theorems if we choose
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
(27)
then we can give some recurrence relations for the family ofmultivariable polynomials given explicitly by (3) In the viewof Theorem 6 we get
Corollary 8 For the family of multivariable polynomialsgenerated by (2) the following relations hold
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
(28)
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Θ(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(29)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also for 119899
119894=
0 1 119898119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 we have
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym) (30)
120597
120597119910119894
Θ(120572)
1198991119899119903
(x ym) = 0 (31)
Corollary 9 By summing the relations given by (28) and (29)respectively for 119894 = 1 2 119903 we get
119903
sum119894=1
119899119894Θ(120572)
1198991119899119903
(x ym)
=119903
sum119894=1
119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus119903
sum119894=1
119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
The Scientific World Journal 5
119903
sum119894=1
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym)
minus119903
sum119894=1
119898119894119910119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
= minus119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(32)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Similarly as a consequence ofTheorem 7 we can give thenext result at once
Corollary 10 Other recurrence relations for the family ofmultivariable polynomials Θ(120572)
1198991119899119903
(x ym) are
minus 119898119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(33)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (34)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Theorem 11 The generating relation (2) yields the followingaddition formula for the family of multivariable polynomialsgiven by (3)
Θ(120572+120573)
1198991119899119903
(x ym) =1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym)
(35)
Proof From (2) we have
infin
sum1198991 119899119903=0
Θ(120572+120573)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus(120572+120573)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
times (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120573
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
timesinfin
sum1198961 119896119903=0
Θ(120573)
1198961 119896119903
(x ym) 11990511989611sdot sdot sdot 119905119896119903
119903
(36)
Replacing 119899119894by 119899
119894minus 119896
119894 119894 = 1 2 119903 the right-hand side of
the last equality is
infin
sum1198991119899119903=0
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(37)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903completes the proof
We now give expansions of the family of multivariablepolynomialsΘ(120572)
1198991119899119903
(x ym) given explicitly by (3) in series ofLegendre Gegenbauer Hermite and Laguerre polynomials
Theorem 12 Expansions of Θ(120572)
1198991119899119903
(x ym) in series of Leg-endre Gegenbauer Hermite and Laguerre polynomials are asfollows
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus119898119894119896119894minus119904119894
times(minus1)119896119894119910119896119894119894119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 119898
119894119896119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus119898119894119896119894minus119904119894+1
times(minus119910119894)119896119894119862]119894
119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898i]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(minus119910119894)119896119894119867
119899119894minus119898119894119896119894minus2119904119894(119898
1198941199091198942)
119896119894119904119894 (119899
119894minus 119898
119894119896119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
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Applied MathematicsJournal of
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Mathematical PhysicsAdvances in
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Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
4 The Scientific World Journal
Proof Fix 119894 = 1 2 119903 Then by differentiating (16) withrespect to 119909
119894and 119905
119894 after making necessary calculations we
obtain thatinfin
sum1198991119899119903=0
119899119894Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (119909119894minus 119910
119894119905119898119894minus1119894
)infin
sum1198991119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119909119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
minus 119910119894
infin
sum1198991 119899119894minus1119899119894+1119899119903=0
(119899119894ge119898119894minus1)
120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
times 11990511989911sdot sdot sdot 119905119899119903
119903
(21)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain (17) and
(18) for the fixed 119894 Similarly if we differentiate (16) withrespect to 119910
119894and 119905
119894 we can find the relation (19)
Theorem 7 If Ψ1198991119899119903
(x ym) is a family of functions gener-ated by (16) then it satisfies the relations
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(22)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (23)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Proof By comparing the derivatives of (16) with respect to 119909119894
and 119910119894 we have
minus 119898119894119905119894
infin
sum1198991 119899119903=0
120597
120597119910119894
Ψ1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= 119905119898119894119894
infin
sum1198991 119899119903=0
120597
120597119909119894
Ψ1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(24)
which implies that
minus 119898119894
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Ψ1198991119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(25)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Ψ1198991119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (26)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Thus
the proof is completed
As a result of these theorems if we choose
119866 (119898111990911199051minus 119910
111990511989811 119898
119903119909119903119905119903minus 119910
119903119905119898119903119903)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
(27)
then we can give some recurrence relations for the family ofmultivariable polynomials given explicitly by (3) In the viewof Theorem 6 we get
Corollary 8 For the family of multivariable polynomialsgenerated by (2) the following relations hold
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus 119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
(28)
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym) minus 119898119894119910119894
120597
120597119910119894
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
= minus (119899119894minus 119898
119894+ 1)Θ(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(29)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 Also for 119899
119894=
0 1 119898119894minus 2 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 we have
119899119894Θ(120572)
1198991 119899119903
(x ym) = 119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym) (30)
120597
120597119910119894
Θ(120572)
1198991119899119903
(x ym) = 0 (31)
Corollary 9 By summing the relations given by (28) and (29)respectively for 119894 = 1 2 119903 we get
119903
sum119894=1
119899119894Θ(120572)
1198991119899119903
(x ym)
=119903
sum119894=1
119909119894
120597
120597119909119894
Θ(120572)
1198991119899119903
(x ym)
minus119903
sum119894=1
119910119894
120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(x ym)
The Scientific World Journal 5
119903
sum119894=1
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym)
minus119903
sum119894=1
119898119894119910119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
= minus119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(32)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Similarly as a consequence ofTheorem 7 we can give thenext result at once
Corollary 10 Other recurrence relations for the family ofmultivariable polynomials Θ(120572)
1198991119899119903
(x ym) are
minus 119898119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(33)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (34)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Theorem 11 The generating relation (2) yields the followingaddition formula for the family of multivariable polynomialsgiven by (3)
Θ(120572+120573)
1198991119899119903
(x ym) =1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym)
(35)
Proof From (2) we have
infin
sum1198991 119899119903=0
Θ(120572+120573)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus(120572+120573)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
times (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120573
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
timesinfin
sum1198961 119896119903=0
Θ(120573)
1198961 119896119903
(x ym) 11990511989611sdot sdot sdot 119905119896119903
119903
(36)
Replacing 119899119894by 119899
119894minus 119896
119894 119894 = 1 2 119903 the right-hand side of
the last equality is
infin
sum1198991119899119903=0
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(37)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903completes the proof
We now give expansions of the family of multivariablepolynomialsΘ(120572)
1198991119899119903
(x ym) given explicitly by (3) in series ofLegendre Gegenbauer Hermite and Laguerre polynomials
Theorem 12 Expansions of Θ(120572)
1198991119899119903
(x ym) in series of Leg-endre Gegenbauer Hermite and Laguerre polynomials are asfollows
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus119898119894119896119894minus119904119894
times(minus1)119896119894119910119896119894119894119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 119898
119894119896119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus119898119894119896119894minus119904119894+1
times(minus119910119894)119896119894119862]119894
119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898i]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(minus119910119894)119896119894119867
119899119894minus119898119894119896119894minus2119904119894(119898
1198941199091198942)
119896119894119904119894 (119899
119894minus 119898
119894119896119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
The Scientific World Journal 5
119903
sum119894=1
119898119894119909119894
120597
120597119910119894
Θ(120572)
1198991 119899119903
(x ym)
minus119903
sum119894=1
119898119894119910119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
= minus119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times Θ(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(x ym)
(32)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Similarly as a consequence ofTheorem 7 we can give thenext result at once
Corollary 10 Other recurrence relations for the family ofmultivariable polynomials Θ(120572)
1198991119899119903
(x ym) are
minus 119898119894
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1 119899119903
(x ym)
=120597
120597119909119894
Θ(120572)
1198991 119899119894minus1119899119894minus119898119894 119899119894+1119899119903
(x ym)
(33)
for 119899119894ge 119898
119894 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894 and
120597
120597119910119894
Θ(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(x ym) = 0 (34)
for 119899119894= 1 2 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Theorem 11 The generating relation (2) yields the followingaddition formula for the family of multivariable polynomialsgiven by (3)
Θ(120572+120573)
1198991119899119903
(x ym) =1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym)
(35)
Proof From (2) we have
infin
sum1198991 119899119903=0
Θ(120572+120573)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus(120572+120573)
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
times (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120573
=infin
sum1198991 119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
timesinfin
sum1198961 119896119903=0
Θ(120573)
1198961 119896119903
(x ym) 11990511989611sdot sdot sdot 119905119896119903
119903
(36)
Replacing 119899119894by 119899
119894minus 119896
119894 119894 = 1 2 119903 the right-hand side of
the last equality is
infin
sum1198991119899119903=0
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
Θ(120572)
1198991minus1198961 119899119903minus119896119903
(x ym)
times Θ(120573)
1198961 119896119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
(37)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903completes the proof
We now give expansions of the family of multivariablepolynomialsΘ(120572)
1198991119899119903
(x ym) given explicitly by (3) in series ofLegendre Gegenbauer Hermite and Laguerre polynomials
Theorem 12 Expansions of Θ(120572)
1198991119899119903
(x ym) in series of Leg-endre Gegenbauer Hermite and Laguerre polynomials are asfollows
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus119898119894119896119894minus119904119894
times(minus1)119896119894119910119896119894119894119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 119898
119894119896119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus119898119894119896119894minus119904119894+1
times(minus119910119894)119896119894119862]119894
119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898i]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(minus119910119894)119896119894119867
119899119894minus119898119894119896119894minus2119904119894(119898
1198941199091198942)
119896119894119904119894 (119899
119894minus 119898
119894119896119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
6 The Scientific World Journal
Θ(120572)
1198991 119899119903
(x ym)
=119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
119899119894minus119898119894119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus119898119894119896119894
2119899119894minus119898119894119896119894(minus1)119904119894
119896119894 (119899
119894minus 119898
119894119896119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus119910119894)119896119894119871(120573119894)
119904119894
(119898119894119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
(38)
Proof By (2) we get
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
= (1 minus119903
sum119894=1
(119898119894119909119894119905119894minus 119910
119894119905119898119894119894))
minus120572
=infin
sum1198991 119899119903=0
infin
sum1198961 119896119903=0
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903(minus1)1198961+sdotsdotsdot+119896119903
times (11989811199091)1198991 sdot sdot sdot (119898
119903119909119903)1198991199031199101198961
1sdot sdot sdot 119910119896119903
119903
times 1199051198991+119898111989611
sdot sdot sdot 119905119899119903+119898119903119896119903119903
(39)
If we use the result in [11 page 181]
(119898119909)119899
119899=
[1198992]
sum119904=0
(2119899 minus 4119904 + 1) 119875119899minus2119904
(1198981199092)
119904(32)119899minus119904
(40)
we can write that
infin
sum1198991119899119903=0
Θ(120572)
1198991 119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=119903
prod119894=1
infin
sum119899119894=0
infin
sum119896119894=0
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119898119894119909119894
2)
times(minus119910119894)119896119894119905119899119894+119898119894119896119894
119894
(120572)1198991+sdotsdotsdot+119899119903+1198961+sdotsdotsdot+119896119903
(41)
Getting 119899119894minus 119898
119894119896119894instead of 119899
119894in the last equality we have
infin
sum1198991 119899119903=0
Θ(120572)
1198991119899119903
(x ym) 11990511989911sdot sdot sdot 119905119899119903
119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894119905119899119894
119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
=infin
sum1198991 119899119903=0
119903
prod119894=1
[119899119894119898119894]
sum119896119894=0
[(119899119894minus119898119894119896119894)2]
sum119904119894=0
(2119899119894minus 2119898
119894119896119894minus 4119904
119894+ 1)
119904119894119896119894(32)
119899119894minus119898119894119896119894minus119904119894
times119875119899119894minus119898119894119896119894minus2119904119894
(119898119894119909119894
2) (minus119910
119894)119896119894
times (120572)1198991+sdotsdotsdot+119899119903minus(1198981minus1)1198961minussdotsdotsdotminus(119898119903minus1)119896119903
11990511989911sdot sdot sdot 119905119899119903
119903
(42)
Comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903gives the desired
relationIn a similar manner in (39) using the following results
respectively [11 page 283 (36) page 194 (4) page 207 (2)]
(119898119909)119899
119899=
[1198992]
sum119896=0
(] + 119899 minus 2119896) 119862]119899minus2119896
(1198981199092)
119896(])119899+1minus119896
(119898119909)119899
119899=
[1198992]
sum119896=0
119867119899minus2119896
(1198981199092)
119896 (119899 minus 2119896)
(119898119909)119899
119899= 2119899
119899
sum119896=0
(minus1)119896(120572 + 1)119899119871(120572)119896
(1198981199092)
(119899 minus 119896)(120572 + 1)119896
(43)
one can easily obtain the other expansions ofΘ(120572)
1198991 119899119903
(x ym)in series of Gegenbauer Hermite and Laguerre polynomials
5 The Special Cases of Θ(120572)
119899(x y m) and
Some Properties
In this section we discuss some special cases of the family ofmultivariable polynomialsΘ(120572)
119899(x ym) and give their several
properties
51TheCase of119898119894= 2 119910
119894= 1 119894 = 1 2 119903 in (2) This case
gives a multivariable analogue of Gegenbauer polynomials
(1 minus 211990911199051+ 1199052
1minus sdot sdot sdot minus 2119909
119903119905119903+ 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
119862(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(44)
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Differential EquationsInternational Journal of
Volume 2014
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Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Discrete Dynamics in Nature and Society
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
The Scientific World Journal 7
which reduces to two variables Gegenbauer polynomialsgiven by [12] for 119903 = 2 Equation (44) yields the followingformula
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
)
times (1198961 sdot sdot sdot 119896
119903 (119899
1minus 2119896
1)
sdot sdot sdot (119899119903minus 2119896
119903))
minus1
)
times (minus1)1198961+sdotsdotsdot+119896119903(21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
(45)
It follows that 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of
degree 119899119894with respect to the fixed variable 119909
119894(119894 = 1 2 119903)
Thus 119862(120572)
1198991 119899119903
(1199091 119909
119903) is a polynomial of total degree (119899
1+
sdot sdot sdot+119899119903)with respect to the variables 119909
1 119909
119903 Equation (45)
also yields
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=21198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
11990911989911sdot sdot sdot 119909119899119903
119903+ Π (119909
1 119909
119903)
(46)
whereΠ(1199091 119909
119903) is a polynomial of degree (119899
1+ sdot sdot sdot + 119899
119903minus
2) with respect to the variables 1199091 119909
119903 In (44) by getting
1199091rarr minus119909
1and 119905
1rarr minus119905
1 we have
119862(120572)
1198991 119899119903
(minus1199091 119909
2 119909
119903) = (minus1)1198991119862(120572)
1198991 119899119903
(1199091 119909
119903)
(47)
Similarly for 119894 = 1 2 119903 we get
119862(120572)
1198991 119899119903
(1199091 119909
119894minus1 minus119909
119894 119909
119894+1 119909
119903)
= (minus1)119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
(48)
Taking 119909119894rarr minus119909
119894and 119905
119894rarr minus119905
119894 119894 = 1 2 119903 in (44)
we obtain
119862(120572)
1198991 119899119903
(minus1199091 minus119909
119903) = (minus1)1198991+sdotsdotsdot+119899119903119862(120572)
1198991 119899119903
(1199091 119909
119903)
(49)
Theorem 13 For the polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) one has
119862(120572)
21198991 2119899119903
(0 0 0) =(minus1)1198991+sdotsdotsdot+119899119903(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903
(50)
and if at least one of 119899119894 119894 = 1 2 119903 is odd then
119862(120572)
1198991 119899119903
(0 0 0) = 0 (51)
Proof If we set all 119909119894= 0 119894 = 1 2 119903 in (44) we have
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991119899119903=0
119862(120572)
1198991 119899119903
(0 0 0) 11990511989911sdot sdot sdot 119905119899119903
119903
(52)
On the other hand we get
(1 + 11990521+ sdot sdot sdot + 1199052
119903)minus120572
=infin
sum1198991 119899119903=0
(minus1)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(120572)
1198991+sdotsdotsdot+119899119903119905211989911
sdot sdot sdot 1199052119899119903119903
(53)
By comparing the coefficients of 11990511989911sdot sdot sdot 119905119899119903
119903 we obtain the
desired
From the theorems and corollaries given in Section 4 wecan give some other properties of 119862(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 14 ByCorollaries 8 and 9 for the family ofmultivari-able polynomials generated by (44) the following relations
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
= 119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119899119894119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119862(120572)
1198991 119899119903
(1199091 119909
119903)
minus119903
sum119894=1
120597
120597119909119894
119862(120572)
1198991 119899119894minus1119899119894minus1119899119894+1119899119903
(1199091 119909
119903)
(54)
hold for 119899119894ge 1 119894 = 1 2 119903
Remark 15 FromTheorem 11 the multivariable polynomials119862(120572)
1198991 119899119903
(1199091 119909
119903) satisfy the following addition formula
119862(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119862(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119862(120573)
1198961 119896119903
(1199091 119909
119903)
(55)
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
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Stochastic AnalysisInternational Journal of
8 The Scientific World Journal
Remark 16 As a result of Theorem 12 expansions of 119862(120572)
1198991 119899119903
(1199091 119909
119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are as follows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(2119899119894minus 4119896
119894minus 4119904
119894+ 1)
119896119894119904119894(32)
119899119894minus2119896119894minus119904119894
times(minus1)119896119894119875119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(]119894+ 119899
119894minus 2119896
119894minus 2119904
119894)
119896119894119904119894(]
119894)119899119894minus2119896119894minus119904119894+1
times(minus1)119896119894119862]119894119899119894minus2119896119894minus2119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
[(119899119894minus2119896119894)2]
sum119904119894=0
(minus1)119896119894119867119899119894minus2119896119894minus2119904119894
(119909119894)
119896119894119904119894 (119899
119894minus 2119896
119894minus 2119904
119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119896119894=0
119899119894minus2119896119894
sum119904119894=0
(120573119894+ 1)
119899119894minus2119896119894
2119899119894minus2119896119894(minus1)119904119894
119896119894 (119899
119894minus 2119896
119894minus 119904
119894)(120573
119894+ 1)
119904119894
times(minus1)119896119894119871(120573119894)119904119894
(119909119894)
times (120572)1198991+sdotsdotsdot+119899119903minus1198961minussdotsdotsdotminus119896119903
(56)
We now give a hypergeometric representation for themultivariable polynomials 119862(120572)
1198991 119899119903
(1199091 119909
119903) given by (44)
Theorem 17 The multivariable polynomials 119862(120572)
1198991 119899119903
(1199091
119909119903) have the following hypergeometric representation
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
times 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
(max 1
11990921
1
1199092119903
lt 1)
(57)
where 119865(119903)119861
is a Lauricella function of 119903-variable defined by [13](see also [2])
119865(119903)119861
[1198861 119886
119903 1198871 119887
119903 119888 119909
1 119909
119903]
=infin
sum1198991119899119903=0
(1198861)1198991
sdot sdot sdot (119886119903)119899119903
(1198871)1198991
sdot sdot sdot (119887119903)119899119903
(119888)1198991+sdotsdotsdot+119899119903
11990911989911
1198991sdot sdot sdot
119909119899119903119903
119899119903
(max 100381610038161003816100381611990911003816100381610038161003816
10038161003816100381610038161199091199031003816100381610038161003816 lt 1)
(58)
Proof We have the following results from [11]
(120572)119899minus119896
=(minus1)119896(120572)
119899
(1 minus 120572 minus 119899)119896
(minus119899)2119896
= 22119896(minus119899
2)119896
(minus119899 + 1
2)119896
(119899 minus 2119896) =119899
(minus119899)2119896
(59)
In view of these relations the equality (45) can be written asfollows
119862(120572)
1198991 119899119903
(1199091 119909
119903)
=[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((120572)1198991+sdotsdotsdot+119899119903
22(1198961+sdotsdotsdot+119896119903)(minus1198991
2)1198961
times (minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
times(minus119899
119903+ 1
2)119896119903
)
times (1198961 sdot sdot sdot 119896
1199031198991 sdot sdot sdot 119899
119903
times (1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
)minus1
)
times (21199091)1198991minus21198961 sdot sdot sdot (2119909
119903)119899119903minus2119896119903
=(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Mathematical PhysicsAdvances in
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OptimizationJournal of
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International Journal of
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Operations ResearchAdvances in
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Decision SciencesAdvances in
Discrete MathematicsJournal of
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Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
The Scientific World Journal 9
times[11989912]
sum1198961=0
sdot sdot sdot[1198991199032]
sum119896119903=0
(((minus1198991
2)1198961
(minus119899
1+ 1
2)1198961
sdot sdot sdot (minus119899119903
2)119896119903
(minus119899
119903+ 1
2)119896119903
)
times ((1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
119903)1198961+sdotsdotsdot+119896119903
times 1198961 sdot sdot sdot 119896
119903)
minus1
)
times(1
11990921
)1198961
sdot sdot sdot (1
1199092119903
)119896119903
= 119865(119903)119861
[ minus1198991
2 minus
119899119903
2minus119899
1+ 1
2
minus119899119903+ 1
2
1 minus 120572 minus 1198991minus sdot sdot sdot minus 119899
1199031
11990921
1
1199092119903
]
times(120572)
1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
119903(2119909
1)1198991 sdot sdot sdot (2119909
119903)119899119903
(60)
wheremax 111990921 11199092
119903 lt 1The proof is completed
Remark 18 For 119903 = 2 Theorem 17 reduces to the knownresult for two variable Gegenbauer polynomials given by [12]
52 The Case of 119909119894= 0 119910
119894= minus119909
119894 119894 = 1 2 119903 in (2) This
case yields
(1 minus 119909111990511989811
minus 119909211990511989822
minus sdot sdot sdot minus 119909119903119905119898119903119903)minus120572
=infin
sum1198991 119899119903=0
119880(120572)
1198991119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(61)
which is a different unification from that in [8]
Remark 19 FromCorollaries 8 and 9 the multivariable poly-nomials 119880(120572)
1198991119899119903
(1199091 119909
119903) satisfy
119898119894119909119894
120597
120597119909119894
119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
= (119899119894minus 119898
119894+ 1)119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
119903
sum119894=1
119898119894119909119894
120597
120597119909119894
times 119880(120572)
1198991 119899119894minus1119899119894minus119898119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119898
119894+ 1)
times 119880(120572)
1198991119899119894minus1119899119894minus119898119894+1119899119894+1119899119903
(1199091 119909
119903)
(62)
for 119899119894ge 119898
119894minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 20 As result of Theorem 11 the multivariable poly-nomials 119880(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition for-
mula
119880(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119880(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119880(120573)
1198961 119896119903
(1199091 119909
119903)
(63)
521 The Case of 119898119894= 1 119894 = 1 2 119903 in Section 52 In
this case we get a 119903-variable analogue of Lagrange polyno-mials (see [14]) which is different from that in [10]
(1 minus 11990911199051minus sdot sdot sdot minus 119909
119903119905119903)minus120572
=infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(64)
They are given explicitly by
119866(120572)
1198991 119899119903
(1199091 119909
119903) =
(120572)1198991+sdotsdotsdot+119899119903
1198991 sdot sdot sdot 119899
11990311990911989911sdot sdot sdot 119909119899119903
119903 (65)
Remark 21 From Corollaries 8 and 9 the multivariablepolynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903) = 119909
119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903) (66)
for 119894 = 1 2 119903 and119903
sum119894=1
119899119894119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
sum119894=1
119909119894
120597
120597119909119894
119866(120572)
1198991 119899119903
(1199091 119909
119903)
(67)
Remark 22 By Theorem 11 the multivariable polynomials119866(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119866(120572+120573)
1198991 119899119903
(1199091 119909
119903) =
1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119866(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119866(120573)
1198961 119896119903
(1199091 119909
119903)
(68)
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
10 The Scientific World Journal
Remark 23 From Theorem 12 expansions of 119866(120572)
1198991 119899119903
(1199091
119909119903) in series of Legendre Gegenbauer Hermite and
Laguerre polynomials are given by
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(2119899119894minus 4119904
119894+ 1)
119904119894(32)
119899119894minus119904119894
119875119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
(]119894+ 119899
119894minus 2119904
119894)
119904119894(]
119894)119899119894minus119904119894+1
119862]119894119899119894minus2119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
[1198991198942]
sum119904119894=0
119867119899119894minus2119904119894
(1199091198942)
119904119894 (119899
119894minus 2119904
119894) (120572)
1198991+sdotsdotsdot+119899119903
119866(120572)
1198991 119899119903
(1199091 119909
119903)
=119903
prod119894=1
119899119894
sum119904119894=0
(120573119894+ 1)
119899119894
2119899119894(minus1)119904119894
(119899119894minus 119904
119894)(120573
119894+ 1)
119904119894
119871(120573119894)119904119894
(119909119894
2)
times (120572)1198991+sdotsdotsdot+119899119903
(69)
We can discuss some generating functions for the multi-variable polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903)
Theorem 24 For the polynomials 119866(120572)
1198991 119899119903
(1199091 119909
119903) the
following generating function holds true for 119896 isin N0
infin
sum1198991 119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119896)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(70)
for each 119894 = 1 2 119903 where
[119896]119898= 119896 (119896 minus 1) sdot sdot sdot (119896 minus 119898 + 1) 119898 isin N [119896]
0= 1 (71)
and g (120572120573)
119899(119909 119910) denotes the classical Lagrange polynomials
defined by [14]
(1 minus 119909119905)minus120572(1 minus 119910119905)minus120573
=infin
sum119899=0
g (120572120573)
119899(119909 119910) 119905119899
(120572 120573 isin C |119905| lt min |119909|minus1 10038161003816100381610038161199101003816100381610038161003816minus1
)
(72)
Proof Fix 119894 = 1 2 119903 LetC120585119894andClowast
120585119894
denote the circles ofradius 120576
119894 centered 120585
119894= 119911
119894and 120585
119894= 0 respectively where
0 lt 120576119894lt 1003816100381610038161003816119909119894
1003816100381610038161003816minus1
10038161003816100381610038161003816100381610038161003816100381610038161 minus
119903
sum119896=1
119909119896119911119896
1003816100381610038161003816100381610038161003816100381610038161003816 (73)
Here these circles are described in the positive direction ByCauchyrsquos Integral Formula we have
119863119898
119911119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896
119894
=
119898
2120587119894
∮C120585119894
120585119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119894120585119894minus sdot sdot sdot minus 119909
119903119911119903)minus120572
(120585119894minus 119911
119894)119898+1
119889120585119894
=
119898
2120587119894
times∮Clowast120585119894
(120585119894+ 119911
119894)119896
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119894(120585119894+ 119911
119894) minus sdot sdot sdot minus 119909
119903119911119903)minus120572
120585119898+1
119894
119889120585119894
=
119898
2120587119894
119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times∮Clowast120585119894
(1 + 120585119894119911
119894)119896
120585119898+1
119894
(1 minus
119909119894120585119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
)
minus120572
119889120585119894
= 119898119911119896
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus
1
119911119894
)
= 119898119911119896minus119898
119894(1 minus 119909
11199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
timesg(120572minus119896)119898
(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(74)
On the other hand we can write that
119863119898
119911119894
(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
119911119896119894
= 119863119898
119911119894
119911119896119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
=infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903)119889119898
119889119911119898119894
11991111989911sdot sdot sdot 119911119899119894+119896
119894sdot sdot sdot 119911119899119903
119903
= 119911119896minus119898119894
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
(75)
From (74) and (75) we see that
infin
sum1198991119899119903=0
119866(120572)
1198991 119899119903
(1199091 119909
119903) [119896 + 119899
119894]11989811991111989911sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g(120572minus119896)119898
(119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(76)
Corollary 25 From (71) one observes that
[119899119894+ 119898]
119898= (119899
119894+ 119898) (119899
119894+ 119898 minus 1) sdot sdot sdot (119899
119894+ 1)
= (119899119894+ 1)
119898
(77)
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
The Scientific World Journal 11
for each 119894 = 1 2 119903 By setting 119896 = 119898 in (70) and then using(77) one has
infin
sum1198991 119899119903=0
(119899119894+ 1)
119898119866(120572)
1198991 119899119903
(1199091 119909
119903) 1199111198991
1sdot sdot sdot 119911119899119903
119903
= 119898(1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903)minus120572
times g (120572minus119898)
119898(
119909119894119911119894
1 minus 11990911199111minus sdot sdot sdot minus 119909
119903119911119903
minus1)
(78)
522TheCase of119898119894= 119894 119894 = 1 2 119903 in Section 52 This case
reduces to a multivariable analogue of Lagrange-Hermitepolynomials
(1 minus 11990911199051minus 119909
211990522minus sdot sdot sdot minus 119909
119903119905119903119903)minus120572
=infin
sum1198991119899119903=0
119867(120572)
1198991 119899119903
(1199091 119909
119903) 1199051198991
1sdot sdot sdot 119905119899119903
119903
(79)
which is different from that in [6]
Remark 26 By Corollaries 8 and 9 the multivariable polyno-mials119867(120572)
1198991 119899119903
(1199091 119909
119903) satisfy
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
= (119899119894minus 119894 + 1)119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
119903
sum119894=1
119894119909119894
120597
120597119909119894
119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
=119903
sum119894=1
(119899119894minus 119894 + 1)
times 119867(120572)
1198991 119899119894minus1119899119894minus119894+1119899119894+1 119899119903
(1199091 119909
119903)
(80)
for 119899119894ge 119894 minus 1 119894 = 1 2 119903 119899
119895ge 0 119895 = 119894
Remark 27 FromTheorem 11 the multivariable polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903) have the following addition formula
119867(120572+120573)
1198991119899119903
(1199091 119909
119903)
=1198991
sum1198961=0
sdot sdot sdot119899119903
sum119896119903=0
119867(120572)
1198991minus1198961 119899119903minus119896119903
(1199091 119909
119903)
times 119867(120573)
1198961 119896119903
(1199091 119909
119903)
(81)
Furthermore setting 119898119894
= 119894 119909119894
= 0 119910119894
= minus119909119894
119894 = 1 2 119903 in Corollary 5 we obtain the followingclass of bilinear generating functions for the polynomials119867(120572)
1198991 119899119903
(1199091 119909
119903)
Remark 28 If
Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
=[11989911199011]
sum1198961=0
sdot sdot sdot[119899119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572+120573)
1198991minus11990111198961 119899119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)1199081198961
1sdot sdot sdot 119908119896119903
119903
(82)
where 1198861198961 119896119903
= 0 119901119894isin N 119899
119894 120582
119894 120578
119894isin N
0 119894 = 1 2 119903 and
120582 = (1205821 120582
119903) 120578 = (120578
1 120578
119903)w = (119908
1 119908
119903) then we
have1198991
sum1198971=0
sdot sdot sdot119899119903
sum119897119903=0
[11989711199011]
sum1198961=0
sdot sdot sdot[119897119903119901119903]
sum119896119903=0
1198861198961 119896119903
119867(120572)
1198991minus1198971 119899119903minus119897119903
(1199091 119909
119903)
times 119867(120573)
1198971minus11990111198961 119897119903minus119901119903119896119903
(1199091 119909
119903)
times 119867(120574)
1205821+12057811198961 120582119903+120578119903119896119903
(1199061 119906
119903)
times 1199081198961
1sdot sdot sdot 119908119896119903
119903
= Ξnp120582120578120572120573120574
(1199091 119909
119903 119906
1 119906
119903w)
(83)
References
[1] H W Gould ldquoInverse series relation and other expansionsinvolving Humbert polynomialsrdquo Duke Mathematical Journalvol 32 pp 697ndash711 1965
[2] H M Srivastava and H L A Manocha Treatise on GeneratingFunctions Halsted Press Ellis Horwood Limited John Wileyand Sons Chichester UK 1984
[3] J P Singhal ldquoA note on generalized Humbert polynomialsrdquoGlasnik Matematicki III vol 5 no 25 pp 241ndash245 1970
[4] D Zeitlin ldquoOn a class of polynomials obtained fromgeneralizedHumbert polynomialsrdquo Proceedings of the AmericanMathemat-ical Society vol 18 pp 28ndash34 1967
[5] R Aktas R Sahin and A Altın ldquoOn a multivariable extensionof Humbert polynomialsrdquo Applied Mathematics and Computa-tion vol 218 pp 662ndash666 2011
[6] A Altın and E Erkus ldquoOn a multivariable extension ofthe Lagrange-Hermite polynomialsrdquo Integral Transforms andSpecial Functions vol 17 no 4 pp 239ndash244 2006
[7] A Altın E Erkus and M A Ozarslan ldquoFamilies of linear gen-erating functions for polyno- mials in two variablesrdquo IntegralTransforms and Special Functions vol 17 no 5 pp 315ndash3202006
[8] E Erkus and H M Srivastava ldquoA unfied presentation of somefamilies of multivariable polynomialsrdquo Integral Transforms andSpecial Functions vol 17 pp 267ndash273 2006
[9] E Ozergin M A Ozarslan and H M Srivastava ldquoSome fami-lies of generating functions for a class of bivariate polynomialsrdquoMathematical and Computer Modelling vol 50 pp 1113ndash11202009
[10] W-C C Chan C-J Chyan and H M Srivastava ldquoTheLagrange polynomials in several variablesrdquo Integral Transformsand Special Functions vol 12 no 2 pp 139ndash148 2001
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
12 The Scientific World Journal
[11] E D Rainville Special Functions The Macmillan CompanyNew York NY USA 1960
[12] M A Khan and G S Kahmmash ldquoA study of a two variablesGegenbauer polynomialsrdquo Applied Mathematical Sciences vol2 no 13 pp 639ndash657 2008
[13] G Lauricella ldquoSulle funzioni ipergeometriche a piu variabilirdquoRendiconti del CircoloMatematico di Palermo vol 7 pp 111ndash1581893
[14] A Erdelyi W Magnus F Oberhettinger and F G TricomiHigher Transcendental Functions vol 3 McGraw-Hill BookCompany New York NY USA 1955
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of