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Applied Mathematics and Computation 213 (2009) 554–576
Contents lists available at ScienceDirect
Applied Mathematics and Computation
journal homepage: www.elsevier .com/ locate /amc
Existence of uncountably many bounded nonoscillatory solutionsand their iterative approximations for second order nonlinearneutral delay difference equations
Zeqing Liu a, Shin Min Kang b,*, Jeong Sheok Ume c
a Department of Mathematics, Liaoning Normal University, P.O. Box 200, Dalian, Liaoning 116029, People’s Republic of Chinab Department of Mathematics and the Research Institute of Natural Science, Gyeongsang National University, Jinju 660-701, Republic of Koreac Department of Applied Mathematics, Changwon National University, Changwon 641-773, Republic of Korea
a r t i c l e i n f o a b s t r a c t
Keywords:Second order nonlinear neutral delaydifference equationUncountably many bounded nonoscillatorysolutionsContraction mappingMann iterative sequence with errors
0096-3003/$ - see front matter � 2009 Elsevier Incdoi:10.1016/j.amc.2009.03.050
* Corresponding author.E-mail addresses: [email protected] (Z. Liu), smkan
In this paper, the Banach fixed-point theorem is employed to establish several existenceresults of uncountably many bounded nonoscillatory solutions for the second order nonlin-ear neutral delay difference equation
. All righ
g@nong
D aðnÞD xðnÞ þ bðnÞxðn� sÞð Þ½ � þ Dhðn; xðh1ðnÞÞ; xðh2ðnÞÞ; . . . ; xðhkðnÞÞÞþ f ðn; xðf1ðnÞÞ; xðf2ðnÞÞ; . . . ; xðfkðnÞÞÞ ¼ cðnÞ; n P n0;
where s; k 2 N, n0 2 N0, a; b; c : Nn0 ! R with aðnÞ > 0 for n 2 Nn0 , h; f : Nn0 � Rk ! R andhl; fl : Nn0 ! Z with
limn!1
;hlðnÞ ¼ limn!1
flðnÞ ¼ þ1; l 2 f1;2; . . . ; kg:
A few Mann type iterative approximation schemes with errors are suggested, and the er-rors estimates between the iterative approximations and the nonoscillatory solutions arediscussed. Seven nontrivial examples are given to illustrate the advantages of our results.
� 2009 Elsevier Inc. All rights reserved.
1. Introduction and preliminaries
Within the past 20 years or so, many authors used the fixed point theorems, critical point theory, coincidence degree the-ory, Riccati transformation technique, upper and lower solution method and other nonlinear analysis methods to study theexistence, boundedness, monotonicity, oscillatory, nonoscillatory, asymptotic behavior of solutions or periodic solutions forsome classes of second order neutral delay linear/nonlinear difference equations [1–10,12–23,25].
Li and Saker [8], Li and Zhu [9], Zhang and Li [23] and Zhang and Zhang [25] presented several oscillation criteria for thesecond order advanced functional difference equation
D aðnÞDxðnÞð Þ þ pðnÞxðgðnÞÞ ¼ 0; n P 0; ð1:1Þ
the second order nonlinear difference equation
D aðnÞDxðnÞð Þ þ qðnÞðDxðnÞÞb � pðnÞxaðnÞ ¼ eðnÞ; n P 1; ð1:2Þ
ts reserved.
ae.gsnu.ac.kr (S.M. Kang), [email protected] (J.S. Ume).
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 555
where b and a are ratios of odd positive integers and the second order nonlinear difference equation
D rðn� 1ÞDðxðn� 1Þ þ pðnÞxðn� sÞÞð Þ þ qðnÞxcðn� rÞ ¼ 0; n P 0; ð1:3Þ
where 0 < c < 1 is a quotient of odd positive integers, respectively. Applying the matrix theory and coincidence degree the-ory, Ma et al. [13] established the existence conditions of periodic solutions for the below second order nonlinear differenceequation
D rðnÞDxðn� 1Þð Þ þ f ðn; xðnÞÞ ¼ 0; jnjP 0: ð1:4Þ
Utilizing the Schauder fixed-point theorem, Thandapani et al. [19] investigated the asymptotic behavior of nonoscillatorysolutions for the second order difference equation
D aðnÞDxðnÞð Þ ¼ qðnÞf ðxðnþ 1ÞÞ; n P 0: ð1:5Þ
Recently, Luo and Bainov [12] and Migda and Migda [15] discussed the asymptotic behaviors of nonoscillatory solutions forthe second order neutral difference equation with maxima
D2 xðnÞ þ pðnÞxðn� kÞð Þ þ qðnÞmax xðsÞ : n� l 6 s 6 nf g ¼ 0; n P 1 ð1:6Þ
and the second order neutral difference equation
D2 xðnÞ þ pxðn� kÞð Þ þ f ðn; xðnÞÞ ¼ 0; n P 1; ð1:7Þ
respectively. Very recently, Meng and Yan [14] investigated the existence of bounded nonoscillatory solutions for the secondorder nonlinear and nonautonomous neutral delay difference equation
D2 xðnÞ � pxðn� sÞð Þ ¼Xm
n¼1
qixðn� riÞ þ f ðn; xðn� g1ðnÞÞ; . . . ; xðn� glðnÞÞÞ; n P n0: ð1:8Þ
Jinfa [5] considered the second order neutral delay difference equation with positive and negative coefficients
D2 xðnÞ þ pxðn�mÞð Þ þ pðnÞxðn� kÞ � qðnÞxðn� lÞ ¼ 0; n P n0 ð1:9Þ
and investigated the existence of a nonoscillatory solution of Eq. (1.9) under the condition p–� 1 by using the Banach fixed-point theorem. Employing the cone compression and expansion theorem in Fréchet spaces, Tian and Ge [20] established theexistence of multiple positive solutions of second order discrete equation on the half-line
D2xðn� 1Þ � pDxðn� 1Þ � qxðn� 1Þ þ f ðn; xðnÞÞ ¼ 0; n P 1 ð1:10Þ
with certain boundary value conditions. However, to the best of our knowledge, no work dealing with the existence ofuncountably many nonoscillatory solutions for Eqs. (1.1)–(1.10) and any other second order difference equations has beendone.
In this paper we study the more general second order nonlinear neutral delay difference equation
D aðnÞD xðnÞ þ bðnÞxðn� sÞð Þ½ � þ Dh n; xðh1ðnÞÞ; xðh2ðnÞÞ; . . . ; xðhkðnÞÞð Þþ f n; xðf1ðnÞÞ; xðf2ðnÞÞ; . . . ; xðfkðnÞÞð Þ ¼ cðnÞ; n P n0; ð1:11Þ
where s; k 2 N, n0 2 N0, a; b; c : Nn0 ! R with aðnÞ > 0 for n 2 Nn0 , h; f : Nn0 � Rk ! R and hl; fl : Nn0 ! Z with
limn!1
hlðnÞ ¼ limn!1
flðnÞ ¼ þ1; l 2 f1;2; . . . ; kg:
Applying the Banach fixed-point theorem, we establish sufficient conditions of the existence of uncountably many boundednonoscillatory solutions for Eq. (1.11), suggest a few Mann type iterative approximation methods with errors for thesebounded nonoscillatory solutions and study error estimates between the approximation sequences and the bounded nonos-cillatory solutions.
Throughout this paper, we assume that D is the forward difference operator defined by DxðnÞ ¼ xðnþ 1Þ � xðnÞ,R ¼ ð�1;þ1Þ;Rþ ¼ ½0;þ1Þ, Z and N denote the sets of all integers and positive integers, respectively,
Zt ¼ fn : n 2 Z with n P tg; Nt ¼ fn : n 2 N with n P tg; t 2 Z;
a ¼ inffhlðnÞ; flðnÞ : 1 6 l 6 k;n 2 Nn0g; b ¼minfn0 � s;ag;
l1b represents the Banach space of all bounded sequences on Zb with norm
kxk ¼ supn2Zb
jxðnÞj for x ¼ fxðnÞgn2Zb2 l1b
and
XðN;MÞ ¼ x ¼ fxðnÞgn2Zb2 l1b : N 6 xðnÞ 6 M; n 2 Zb
n ofor M > N > 0:
556 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
It is easy to see that XðN;MÞ is a bounded closed and convex subset of the Banach space l1b . By a solution of Eq. (1.11), wemean a sequence fxðnÞgn2Zb
with a positive integer T P n0 þ sþ jaj such that Eq. (1.11) is satisfied for all n P T. As is cus-tomary, a solution of Eq. (1.11) is said to be oscillatory if it is neither eventually positive nor eventually negative. Otherwise,it is said to be nonoscillatory.
The following lemmas play important roles in this paper.
Lemma 1.1 [11]. Let fangnP0; fbngnP0; fcngnP0 and ftngnP0 be four nonnegative real sequences satisfying the inequality
anþ1 6 ð1� tnÞan þ tnbn þ cn; 8n P 0;
where ftngnP0 � ½0;1�,P1
n¼0tn ¼ þ1, limn!1bn ¼ 0 andP1
n¼0cn < þ1. Then limn!1an ¼ 0.
Lemma 1.2. Let s 2 N, n0 2 N0 and B : Nn0 ! Rþ be a mapping. Then
(a) [24]P1
i¼0
P1s¼n0þisBðsÞ < þ1()
P1n¼n0
nBðnÞ < þ1;
(b)P1
i¼0
P1s¼n0þis
P1t¼sBðtÞ < þ1()
P1s¼n0
P1t¼ssBðtÞ < þ1.
Proof. We only prove (b). For each t 2 R, [t] stands for the largest integer not exceeding t. Note that
X1i¼0
X1s¼n0þis
X1t¼s
BðtÞ ¼X1s¼n0
X1t¼s
BðtÞ þX1
s¼n0þs
X1t¼s
BðtÞ þX1
s¼n0þ2s
X1t¼s
BðtÞ þ � � �
¼X1s¼n0
X1t¼s
1þ s� n0
s
h in oBðtÞ
and
lims!þ1
1þ s�n0s
� �ss
¼ 1:
It follows that (b) holds. This completes the proof. h
The paper is organized as follows. In Section 2, by using the Banach fixed-point theorem, we establish the existence, iter-ative approximations and errors estimates of uncountably many bounded nonoscillatory solutions for Eq. (1.11). The resultspresented in this paper extend properly Theorem 1 in [5]. In Section 3, seven examples are constructed to illustrate ourresults.
2. Existence of uncountably bounded nonoscillatory solutions
Now we study those conditions under which Eq. (1.11) possesses uncountably bounded nonoscillatory solutions. More-over, we suggest a few Mann iterative approximation schemes with errors for these bounded nonoscillatory solutions. Undersuitable conditions, some error estimates between the bounded nonoscillatory solutions and the approximate solutions arediscussed.
Theorem 2.1. Let M and N be two positive constants with M > N and
bðnÞ ¼ �1; eventually: ð2:1Þ
Suppose that there exist four mappings PN;M;Q N;M, RN;M ;WN;M : Nn0 ! Rþ satisfying
jf ðn;u1;u2; . . . ; ukÞ � f ðn; �u1; �u2; . . . ; �ukÞj 6 PN;MðnÞmaxfjul � �ulj : 1 6 l 6 kg;
jhðn;u1;u2; . . . ; ukÞ � hðn; �u1; �u2; . . . ; �ukÞj 6 RN;MðnÞmaxfjul � �ulj : 1 6 l 6 kg
for n 2 Nn0 ; ul; �ul 2 ½N;M� and 1 6 l 6 k; ð2:2Þ
jf ðn;u1;u2; . . . ; ukÞj 6 QN;MðnÞ and jhðn;u1;u2; . . . ;ukÞj 6WN;MðnÞ for n 2 Nn0 ; ul 2 ½N;M� and 1 6 l 6 k; ð2:3Þ
X1n¼n0
naðnÞ max RN;MðnÞ;WN;MðnÞ
� �< þ1; ð2:4Þ
X1s¼n0
X1t¼s
saðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �< þ1: ð2:5Þ
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 557
Then
(a) For any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for each x0 2 XðN;MÞ, the Mann iterative sequencewith errors fxmgmP0 generated by the scheme:
xmþ1ðnÞ ¼
ð1� am � bmÞxmðnÞ þ am L�P1i¼1
P1s¼nþis
1aðsÞ
(
��
hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼s
cðtÞ�)
þ bmcmðnÞ; n P T; m P 0;
ð1� am � bmÞxmðTÞ þ am L�P1i¼1
P1s¼Tþis
1aðsÞ
(
��
hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼s
cðtÞ�)
þbmcmðTÞ; b 6 n < T; m P 0
8>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>><>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>:
ð2:6Þ
converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (1.11) and has the following error estimate:
kxmþ1 � xk 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm; m P 0; ð2:7Þ
where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in ½0;1� such that
X1m¼0
am ¼ þ1 ð2:8Þ
and
X1m¼0
bm < þ1 or there exists a sequence fnmgmP0 # ½0;þ1Þ satisfying bm ¼ nmam; m P 0 and limm!1
nm ¼ 0; ð2:9Þ
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. First of all we show that (a) holds. Let L 2 ðN;MÞ. It follows from (2.1), (2.4), (2.5) and Lemma 1.2 that there existh 2 ð0;1Þ and T P n0 þ sþ jaj satisfying
bðnÞ � �1; n P T; ð2:10Þ
h ¼X1i¼1
X1s¼Tþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
; ð2:11Þ
X1i¼1
X1s¼Tþis
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 min M � L; L� Nf g: ð2:12Þ
Define a mapping SL : XðN;MÞ ! l1b by
SLxðnÞ ¼
L�P1i¼1
P1s¼nþis
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ
�P1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ
þP1t¼s
cðtÞ�; n P T; x 2 XðN;MÞ;
SLxðTÞ; b 6 n < T; x 2 XðN;MÞ:
8>>>>>>>>>>>><>>>>>>>>>>>>:
ð2:13Þ
558 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
Employing (2.2) and (2.11), we infer that for x; y 2 XðN;MÞ and n P T
jSLxðnÞ � SLyðnÞj 6X1i¼1
X1s¼nþis
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
6
X1i¼1
X1s¼nþis
1aðsÞ
�RN;MðsÞmaxfjxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kg
þX1t¼s
PN;MðtÞmaxfjxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kg#
6
X1i¼1
X1s¼nþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
6
X1i¼1
X1s¼Tþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk ¼ hkx� yk:
This leads to
kSLx� SLyk 6 hkx� yk; x; y 2 XðN;MÞ: ð2:14Þ
In view of (2.3), (2.12) and (2.13), we conclude that for any x 2 XðN;MÞ and n P T
SLxðnÞ 6 LþX1i¼1
X1s¼nþis
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
6 LþX1i¼1
X1s¼nþis
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 LþX1i¼1
X1s¼Tþis
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 Lþmin M � L; L� Nf g 6 M
and
SLxðnÞP L�X1i¼1
X1s¼nþis
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
P L�X1i¼1
X1s¼nþis
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L�X1i¼1
X1s¼Tþis
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L�min M � L; L� Nf gP N;
which give that SLðXðN;MÞÞ# XðN;MÞ. Consequently, (2.14) ensures that SL is a contraction mapping and it has a unique fixedpoint x 2 XðN;MÞ, that is,
xðnÞ ¼ L�X1i¼1
X1s¼nþis
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
; n P T
ð2:15Þ
and
xðn� sÞ ¼ L�X1i¼1
X1s¼nþði�1Þs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ;"
xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ#; n P T þ s: ð2:16Þ
Thus (2.10), (2.15) and (2.16) lead to
xðnÞ � xðn� sÞ ¼X1s¼n
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T þ s;
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 559
which yields that
DðxðnÞ � xðn� sÞÞ ¼ � 1aðnÞ hðn; xðh1ðnÞÞ; xðh2ðnÞÞ; . . . ; xðhkðnÞÞÞ �
X1t¼n
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼n
cðtÞ" #
;
n P T þ s;
that is,D aðnÞDðxðnÞ � xðn� sÞÞð Þ ¼ �Dhðn; xðh1ðnÞÞ; xðh2ðnÞÞ; . . . ; xðhkðnÞÞÞ � f ðn; xðf1ðnÞÞ; xðf2ðnÞÞ; . . . ; xðfkðnÞÞÞ þ cðnÞ;n P T þ s;
which means that x a bounded nonoscillatory solution of Eq. (1.11). It follow from (2.6), (2.10), (2.11), (2.13) and (2.14) thatfor any m P 0 and n P T ,
jxmþ1ðnÞ � xðnÞj ¼ ð1� am � bmÞxmðnÞ þ am L�X1i¼1
X1s¼nþis
1aðsÞ hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ½
(������X1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þX1t¼s
cðtÞ#þ bmcmðnÞ � xðnÞ
�����)
6 ð1� am � bmÞjxmðnÞ � xðnÞj þ amjSLxmðnÞ � SLxðnÞj þ bmjcmðnÞ � xðnÞj6 ð1� am � bmÞkxm � xk þ amhkxm � xk þ 2Mbm 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm;
which gives that
kxmþ1 � xk 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm; m P 0:
That is, (2.7) holds. Thus Lemma 1.1, (2.1), (2.8) and (2.9) guarantee that limm!1xm ¼ x.Now we show that (b) holds. By (2.1), (2.4) and (2.5), we know that for any distinct L;K 2 ðN;MÞ, there exist h and
T P n0 þ sþ jaj satisfying (2.10), (2.11), (2.12) and
X1i¼1
X1s¼Tþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
<jL� Kj
2M: ð2:17Þ
Let the mapping SL be defined by (2.13), and define a mapping SK : XðN;MÞ ! l1b by (2.13) with L replaced by K. As in theproof of (a), we conclude easily that the mappings SL and SK have the unique fixed points x; y 2 XðN;MÞ, respectively. Thatis, x and y are bounded nonoscillatory solutions of Eq. (1.11) in XðN;MÞ. In light of (2.13), we deduce that for n P T
xðnÞ ¼ L�X1i¼1
X1s¼nþis
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
; n P T
ð2:18Þ
and " #yðnÞ ¼ K �X1i¼1
X1s¼nþis
1aðsÞ hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞ �
X1t¼s
f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞ þX1t¼s
cðtÞ ; n P T:
ð2:19Þ
It follows from (2.2) and (2.17)–(2.19) that for each n P T
jxðnÞ � yðnÞjP jL� Kj �X1i¼1
X1s¼nþis
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
P jL� Kj �X1i¼1
X1s¼nþis
1aðsÞ
�RN;MðsÞmaxfjxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kg
þX1t¼s
PN;MðtÞmaxfjxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kg#
P jL� Kj �X1i¼1
X1s¼nþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
P jL� Kj � 2MX1i¼1
X1s¼Tþis
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
> 0;
which yields that x – y. This completes the proof. h
560 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
Theorem 2.2. Assume that there exists a constant b 2 ½0;1Þ satisfying
0 6 bðnÞ 6 �b; eventually: ð2:20Þ
Let M and N be two positive constants with ð1� �bÞM > N and there exist four mappings PN;M ;QN;M, RN;M;WN;M : Nn0 ! Rþ satis-fying (2.2) and (2.3),
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �< þ1 ð2:21Þ
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �< þ1: ð2:22Þ
Then
(a) For any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for any x0 2 XðN;MÞ, the Mann iterative sequencewith errors fxmgmP0 generated by the scheme:
xmþ1ðnÞ ¼
ð1� am � bmÞxmðnÞ þ am L� bðnÞxmðn� sÞf
�Pn�1
s¼T
1aðsÞ
�hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼s
cðtÞ�
þbmcmðnÞ; n P T þ 1; m P 0;
ð1� am � bmÞxmðT þ 1Þ þ am L� bðT þ 1ÞxmðT þ 1� sÞf
� 1aðTÞ
�hðT; xmðh1ðTÞÞ; xmðh2ðTÞÞ; . . . ; xmðhkðTÞÞÞ
�P1t¼T
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼T
cðtÞ�
þbmcmðT þ 1Þ; b 6 n 6 T; m P 0
8>>>>>>>>>>>>>>>>>>>>>>>>>>><>>>>>>>>>>>>>>>>>>>>>>>>>>>:
ð2:23Þ
converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (1.11) and satisfies the error estimate (2.7), wherefcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. Set L 2 ðN;MÞ. In view of (2.20)–(2.22), we choice h 2 ð0;1Þ and T P n0 þ sþ jaj such that
0 6 bðnÞ 6 �b; n P T; ð2:24Þ
h ¼ �bþX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
; ð2:25Þ
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6min M � L; L� �bM � N� �
: ð2:26Þ
Define a mapping SL : XðN;MÞ ! l1b by
SLxðnÞ ¼
L� bðnÞxðn� sÞ �Pn�1
s¼T
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ
�P1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ
þP1t¼s
cðtÞ�; n P T þ 1; x 2 XðN;MÞ;
SLxðT þ 1Þ; b 6 n 6 T; x 2 XðN;MÞ:
8>>>>>>>>>>>><>>>>>>>>>>>>:
ð2:27Þ
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 561
By virtue of (2.2), (2.24), (2.25) and (2.27), we gain that for x; y 2 XðN;MÞ and n P T þ 1
jSLxðnÞ � SLyðnÞj 6 bðnÞjxðn� sÞ � yðn� sÞj
þXn�1
s¼T
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
6�bkx� yk þ
Xn�1
s¼T
1aðsÞ
"RN;MðsÞmax jxðhiðsÞÞ � yðhiðsÞÞj : 1 6 i 6 kf g
þX1t¼s
PN;MðtÞmax jxðfiðtÞÞ � yðfiðtÞÞj : 1 6 i 6 kf g#
6�bþ
Xn�1
s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ !" #
kx� yk 6 hkx� yk;
which gives (2.14). Applying (2.3), (2.24), (2.26) and (2.27), we derive that for any x 2 XðN;MÞ and n P T þ 1
SLxðnÞ 6 LþXn�1
s¼T
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
6 LþXn�1
s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
6 LþX1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 Lþmin M � L; L� �bM � N� �
6 M
and
SLxðnÞP L� �bM �Xn�1
s¼T
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
P L� �bM �Xn�1
s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
P L� �bM �X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
P L�min M � L; L� �bM � N� �
P N;
which imply that SLðXðN;MÞÞ# XðN;MÞ. Consequently, (2.14) means that SL is a contraction mapping and it has a uniquefixed point x 2 XðN;MÞ, which is a bounded nonoscillatory solution of Eq. (1.11). Using (2.14), (2.23), (2.25) and (2.27),we infer that for any m P 0 and n P T þ 1,
jxmþ1ðnÞ � xðnÞj ¼ ð1� am � bmÞxmðnÞ þ am L� bðnÞxðn� sÞ �Xn�1
s¼T
1aðsÞ hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ½
(������X1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; � � � ; xmðfkðtÞÞÞ þX1t¼s
cðtÞ#)þ bmcmðnÞ � xðnÞ
�����6 ð1� am � bmÞjxmðnÞ � xðnÞj þ amjSLxmðnÞ � SLxðnÞj þ bmjcmðnÞ � xðnÞj6 ð1� am � bmÞkxm � xk þ amhkxm � xk þ 2Mbm 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm;
which yields that
kxmþ1 � xk 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm; m P 0:
That is, (2.7) holds. Consequently, Lemma 1.1, (2.8) and (2.9) imply that limm!1xm ¼ x. That is, (a) holds.Next we show that (b) holds. By (2.20)–(2.22), we know that for any distinct L;K 2 ðN;MÞ, there exist h 2 ð0;1Þ and
T P n0 þ sþ jaj satisfying (2.24)–(2.26) and
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
<jL� Kj
2M: ð2:28Þ
Let the mapping SL be defined by (2.27), and define a mapping SK : XðN;MÞ ! l1b by (2.27) with L replaced by K. It is easy tocheck that the mappings SL and SK have the unique fixed points x; y 2 XðN;MÞ, respectively. That is, x and y are boundednonoscillatory solutions of Eq. (1.11) in XðN;MÞ. In view of (2.27), we deduce that
562 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
xðnÞ ¼ L� bðnÞxðn� sÞ �Xn�1
s¼T
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T þ 1 ð2:29Þ
andyðnÞ ¼ K � bðnÞyðn� sÞ �Xn�1
s¼T
1aðsÞ hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞ �
X1t¼s
f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T þ 1: ð2:30Þ
Notice that (2.2) together with (2.28)–(2.30) ensures that
jxðnÞ � yðnÞ þ bðnÞðxðn� sÞ � yðn� sÞÞj
P jL� Kj �Xn�1
s¼T
1aðsÞ
"jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
P jL� Kj �Xn�1
s¼T
1aðsÞ RN;MðsÞmaxfjxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kg þ
X1t¼s
PN;MðtÞmaxfjxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kg" #
P jL� Kj �Xn�1
s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
P jL� Kj � 2MX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
> 0; n P T þ 1;
that is, x – y. This completes the proof. h
Theorem 2.3. Assume that there exists a constant b 2 ð�1;0� satisfying
b 6 bðnÞ 6 0; eventually: ð2:31Þ
Let M and N be two positive constants with M > N and there exist four mappings PN;M;Q N;M, RN;M ;WN;M : Nn0 ! Rþ satisfying (2.2),(2.3), (2.21) and (2.22). Then
(a) For any L 2 ðð1þ bÞN; ð1þ bÞMÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for any x0 2 XðN;MÞ, the Mann iter-ative sequence with errors fxmgmP0 generated by (2.23) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq.(1.11) and satisfies the error estimate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 areany sequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. Put L 2 ðð1þ bÞN; ð1þ bÞMÞ. It follows from (2.21), (2.22) and (2.31) that there exist h 2 ð0;1Þ and T P n0 þ sþ jajsatisfying
b 6 bn 6 0; n P T; ð2:32Þ
h ¼ jbj þX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
; ð2:33Þ
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6min ð1þ bÞM � L; L� ð1þ bÞNf g: ð2:34Þ
Define a mapping SL : XðN;MÞ ! l1b by (2.27). Similar to the proof of Theorem 2.2, we conclude that (2.14) holds.Now (2.3), (2.27), (2.32) and (2.34) lead to
SLxðnÞ 6 L� bM þXn�1
s¼T
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
6 L� bM þXn�1
s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 L� bM þX1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
6 L� bM þmin ð1þ bÞM � L; L� ð1þ bÞNf g 6 M; x 2 XðN;MÞ;n P T þ 1
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 563
and
SLxðnÞP L� bN �Xn�1
s¼T
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
P L� bN �Xn�1
s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L� bN �X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L� bN �min ð1þ bÞM � L; L� ð1þ bÞNf gP N; x 2 XðN;MÞ; n P T þ 1;
which imply that SLðXðN;MÞÞ# XðN;MÞ. Consequently, (2.14) means that SL is a contraction mapping and it has a uniquefixed point x 2 XðN;MÞ, which is a bounded nonoscillatory solution of Eq. (1.11). The rest of the proof is similar to that ofTheorem 2.2, and is omitted. This completes the proof. h
Theorem 2.4. Assume that there exist two constants �b and b satisfying
b 6 bðnÞ 6 �b; eventually ð2:35Þ
and1 < b and �b < b2: ð2:36Þ
Let M and N be arbitrary positive constants with M�b b2 � �b �
> Nb �b2 � b �
and there exist four mappings PN;M;Q N;M,RN;M;WN;M : Nn0 ! Rþ satisfying (2.2), (2.3), (2.21) and (2.22). Then
(a) For any L 2 �bN þ �bMb ; bM þ bN
�b
� , there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for each x0 2 XðN;MÞ, the Mann iter-
ative sequence with errors fxmgmP0 generated by the scheme:
xmþ1ðnÞ ¼
ð1� am � bmÞxmðnÞ þ amL
bðnþsÞ �xmðnþsÞbðnþsÞ � 1
bðnþsÞPnþs�1
s¼Tþs
1aðsÞ
�
��
hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ
þP1t¼s
cðtÞ�þ bmcmðnÞ; n P T þ 1; m P 0;
ð1� am � bmÞxmðT þ 1Þ þ am
�L
bðTþ1þsÞ �xmðTþ1þsÞbðTþ1þsÞ � 1
bðTþ1þsÞaðTþsÞ
��
hðT þ s; xmðh1ðT þ sÞÞ; xmðh2ðT þ sÞÞ; . . . ; xmðhkðT þ sÞÞÞ
�P1
t¼Tþsf ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ
þP1
t¼TþscðtÞ
�þ bmcmðT þ 1Þ; b 6 n 6 T; m P 0
8>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>><>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>:
ð2:37Þ
converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (1.11) and has the error estimate (2.7), where fcmgmP0 isan arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. Let L 2 �bN þ �bMb ; bM þ bN
�b
� . In terms of (2.21), (2.22), (2.35) and (2.36), we select h 2 ð0;1Þ and T P n0 þ sþ jaj such
that
b 6 bðnÞ 6 �b; n P T; ð2:38Þ
h ¼ 1b
1þX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #( )
; ð2:39Þ
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6min bM � Lþ bN�b;bL�b�M � bN
� : ð2:40Þ
564 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
Define a mapping SL : XðN;MÞ ! l1b by
SLxðnÞ ¼
LbðnþsÞ �
xðnþsÞbðnþsÞ � 1
bðnþsÞPnþs�1
s¼Tþs
1aðsÞ
��
hðs; xðh1ðbÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ
�P1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ
þP1t¼s
cðtÞ�; n P T þ 1; x 2 XðN;MÞ;
SLxðT þ 1Þ; b 6 n 6 T; x 2 XðN;MÞ:
8>>>>>>>>>>>>>>><>>>>>>>>>>>>>>>:
ð2:41Þ
Thus (2.2), (2.36), (2.38), (2.39) and (2.41) imply that for x; y 2 XðN;MÞ and n P T þ 1
jSLxðnÞ � SLyðnÞj 6 jxðnþ sÞ � yðnþ sÞjbðnþ sÞ þ 1
bðnþ sÞXnþs�1
s¼Tþs
1aðsÞ
��
hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj j
þX1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj j#
6kx� yk
bþ 1
b
Xnþs�1
s¼Tþs
1aðsÞ
"RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
61b
1þX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #( )
kx� yk ¼ hkx� yk;
that is, (2.14) holds. It follows from (2.3), (2.36), (2.38), (2.40) and (2.41) that for any x 2 XðN;MÞ and n P T þ 1
SLxðnÞ 6 Lb� N
�bþ 1
b
Xnþs�1
s¼Tþs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj j þ
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj j þX1t¼s
cðtÞj j" #
6Lb� N
�bþ 1
b
Xnþs�1
s¼Tþs
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
cðtÞj j" #
6Lb� N
�bþ 1
b
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
6Lb� N
�bþ 1
bmin bM � Lþ bN
�b;bL�b�M � bN
� 6 M
and
SLxðnÞP L�b�M
b� 1
b
Xnþs�1
s¼Tþs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj j þ
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj j þX1t¼s
cðtÞj j" #
PL�b�M
b� 1
b
Xnþs�1
s¼Tþs
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
PL�b�M
b� 1
b
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
PL�b�M
b� 1
bmin bM � Lþ bN
�b;bL�b�M � bN
� P N;
which imply that SLðXðN;MÞÞ# XðN;MÞ. Eq. (2.14) gives that SL is a contraction mapping and hence it has a unique fixed pointx 2 XðN;MÞ, which is a bounded nonoscillatory solution of Eq. (1.11). It follows from (2.14), (2.37) and (2.41) that for anym P 0 and n P T þ 1
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 565
jxmþ1ðnÞ � xðnÞj ¼ ð1� am � bmÞxmðnÞ þ amL
bðnþ sÞ �xmðnþ sÞbðnþ sÞ
������ 1
bðnþ sÞXnþs�1
s¼Tþs
1aðsÞ
�hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
þX1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; � � � ; xmðfkðtÞÞÞ þX1t¼s
cðtÞ#)þ bmcmðnÞ � xðnÞ
�����6 ð1� am � bmÞjxmðnÞ � xðnÞj þ amjSLxmðnÞ � SLxðnÞj þ bmjcmðnÞ � xðnÞj6 ð1� am � bmÞkxm � xk þ amhkxm � xk þ 2Mbm
6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm;
which yields (2.7). Thus Lemma 1.1, (2.8) and (2.9) ensure that limm!1xm ¼ x.Now we show that (b) holds. In terms of (2.21), (2.22) and (2.35), we derive that for any distinct L;K 2 �bN þ �bM
b ; bM þ bN�b
� ,
there exist h 2 ð0;1Þ and T P n0 þ sþ jaj satisfying (2.38)–(2.40) and
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
<bjL� Kj
2M�b: ð2:42Þ
Let the mapping SL be defined by (2.41), and define a mapping SK : XðN;MÞ ! l1b by (2.41) with L replaced by K. Obviously,the mappings SL and SK have the unique fixed points x; y 2 XðN;MÞ, respectively. That is, x and y are bounded nonsocillatorysolutions of Eq. (1.11) in XðN;MÞ. In view of (2.41), we conclude that
xðnÞ ¼ Lbðnþ sÞ �
xðnþ sÞbðnþ sÞ �
1bðnþ sÞ
Xnþs�1
s¼Tþs
1aðsÞ
"hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ
�X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ#; n P T þ 1 ð2:43Þ
and
yðnÞ ¼ Kbðnþ sÞ �
yðnþ sÞbðnþ sÞ �
1bðnþ sÞ
Xnþs�1
s¼Tþs
1aðsÞ
"hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞ
�X1t¼s
f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞ þX1t¼s
cðtÞ#; n P T þ 1: ð2:44Þ
Notice that (2.2), (2.36), (2.38) and (2.42), (2.43), (2.44) mean that for n P T þ 1
xðnÞ � yðnÞ þ xðnþ sÞ � yðnþ sÞbðnþ sÞ
��������
PjL� Kj
bðnþ sÞ �1
bðnþ sÞXnþs�1
s¼Tþs
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj j
þX1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtsÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj j#
PjL� Kj
�b� 1
b
Xnþs�1
s¼Tþs
1aðsÞ
�RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
PjL� Kj
�b� 1
b
Xnþs�1
s¼Tþs
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
PjL� Kj
�b� 2M
b
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
> 0;
that is, x – y. This completes the proof. h
Theorem 2.5. Assume that there exist two constants �b and b satisfying (2.35) and
�b < �1: ð2:45Þ
Let M and N be arbitrary positive constants with MN >
1þb1þ�b
and there exist four mappings PN;M ;Q N;M, RN;M;WN;M : Nn0 ! Rþ satisfying(2.2), (2.3), (2.21) and (2.22). Then
566 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
(a) For any L 2 Mð1þ �bÞ;Nð1þ bÞ �
, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for each x0 2 XðN;MÞ, the Mann iter-ative sequence with errors fxmgmP0 generated by (2.37) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq.(1.11) and has the error estimate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are anysequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. First of all we show (a). Taking L 2 Mb 1þ 1�b
� ;N�b 1þ 1
b
� � , from (2.21), (2.35) and (2.45), we infer that there exist
h 2 ð0;1Þ and T P n0 þ sþ jaj satisfying (2.38),
h ¼ �1�b
1þX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #( )
ð2:46Þ
and
X1s¼T1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
6 min L�Mð1þ �bÞ; �b N 1þ 1b
� �� L
b
� �� : ð2:47Þ
Let the mapping SL : XðN;MÞ ! l1b be defined by (2.41). It follows from (2.2), (2.38), (2.41), (2.45) and (2.46) that forx; y 2 XðN;MÞ and n P T þ 1
jSLxðnÞ � SLyðnÞj 6 � jxðnþ sÞ � yðnþ sÞjbðnþ sÞ � 1
bðnþ sÞ
�Xnþs�1
s¼Tþs
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj j
þX1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj j#
6 �kx� yk�b
� 1�b
Xnþs�1
s¼Tþs
1aðsÞ
�RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
6 �1�b
1þX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #( )
kx� yk ¼ hkx� yk:
Hence (2.14) holds. By means of (2.3), (2.38), (2.41), (2.45) and (2.47), we gain that for any x 2 XðN;MÞ and n P T þ 1
SLxðnÞ 6 L�b�M
�b� 1
�b
Xnþs�1
s¼Tþs
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj j
þX1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj j þX1t¼s
cðtÞj j#
6L�b�M
�b� 1
�b
Xnþs�1
s¼Tþs
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
6L�b�M
�b� 1
�b
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
6L�b�M
�b� 1
�bmin L�Mð1þ �bÞ; �b N 1þ 1
b
� �� L
b
� �� 6 M
and
SLxðnÞP Lb� N
bþ 1
�b
Xnþs�1
s¼Tþs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj j þ
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj j þX1t¼s
cðtÞj j" #
PLb� N
bþ 1
�b
Xnþs�1
s¼Tþs
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
PLb� N
bþ 1
�b
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
cðtÞj j" #
PLb� N
bþ 1
�bmin L�Mð1þ �bÞ; �b N 1þ 1
b
� �� L
b
� �� P N;
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 567
which imply that SLðXðN;MÞÞ# XðN;MÞ. (2.14) ensures that SL is a contraction mapping and hence it has a unique fixed pointx 2 XðN;MÞ, which is a bounded nonoscillatory solution of Eq. (1.11). As in the proof of Theorem 2.4, we infer that (2.7) holdsand limm!1xm ¼ x.
Next we prove (b). By (2.21), (2.22), (2.35) and (2.45), we get that for any distinct L;K 2 Mð1þ �bÞ;Nð1þ bÞ �
, there existh 2 ð0;1Þ and T > n0 þ sþ jaj satisfying (2.38), (2.46), (2.47) and
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
<�bjL� Kj
2Mb: ð2:48Þ
Let the mapping SL be defined by (2.41), and define a mapping SK : XðN;MÞ ! l1b by (2.41) with L replaced by K. It is easy toverify that the mappings SL and SK have the unique fixed points x; y 2 XðN;MÞ, which satisfy (2.43) and (2.44), respectively,that is, x and y are bounded oscillatory solutions of Eq. (1.11) in XðN;MÞ. Thus (2.35), (2.43)–(2.45) and (2.48) lead to
xðnÞ � yðnÞ þ xðnþ sÞ � yðnþ sÞbðnþ sÞ
��������
P � jL� Kjbðnþ sÞ þ
1bðnþ sÞ
Xnþs�1
s¼Tþs
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj j
þX1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj j#
P � jL� Kjbþ 1
�b
Xnþs�1
s¼Tþs
1aðsÞ
�RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
P � jL� Kjbþ 1
�b
Xnþs�1
s¼Tþs
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
P � jL� Kjbþ 2M
�b
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
> 0
for n P T þ 1. That is, x–y. This completes the proof. h
Theorem 2.6. Assume that
bðnÞ ¼ 1; eventually: ð2:49Þ
Let M and N be two positive constants with M > N and there exist four mappings PN;M;Q N;M, RN;M;WN;M : Nn0 ! Rþ satisfying (2.2),(2.3), (2.21) and (2.22). Then(a) For any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for each x0 2 XðN;MÞ, the Mann iterative sequencewith errors fxmgmP0 generated by the scheme:
xmþ1ðnÞ ¼
ð1� am � bmÞxmðnÞ þ am LþP1i¼1
Pnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
(
��
hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼s
cðtÞ�
þbmcmðnÞ; n P T; m P 0;
ð1� am � bmÞxmðTÞ þ am LþP1i¼1
PTþ2is�1
s¼Tþð2i�1Þs
1aðsÞ
(
��
hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ
�P1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þP1t¼s
cðtÞ�
þbmcmðTÞ; b 6 n < T; m P 0
8>>>>>>>>>>>>>>>>>>>>>>>>>>>>>><>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>:
ð2:50Þ
converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (1.11) and has the error estimate (2.7), where fcmgmP0 isan arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
568 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
Proof. First of all we show that (a) holds. Let L 2 ðN;MÞ. It follows from (2.21), (2.22), (2.49) that there exist h 2 ð0;1Þ andT P n0 þ sþ jaj satisfying
bðnÞ � 1; n P T ð2:51Þ
h ¼X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
; ð2:52Þ
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6min M � L; L� Nf g: ð2:53Þ
Define a mapping SL : XðN;MÞ ! l1b by
SLxðnÞ ¼
LþP1i¼1
Pnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
�hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ
�P1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ
þP1t¼s
cðtÞ�; n P T; x 2 XðN;MÞ;
SLxðTÞ; b 6 n < T; x 2 XðN;MÞ:
8>>>>>>>>>><>>>>>>>>>>:
ð2:54Þ
On account of (2.2), (2.52) and (2.54), we derive that for x; y 2 XðN;MÞ and n P T
jSLxðnÞ � SLyðnÞj 6X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
6
X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
�RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
6
X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
6
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk ¼ hkx� yk;
which yields (2.14). By means of (2.3), (2.53) and (2.54), we gain that for any x 2 XðN;MÞ and n P T
SLxðnÞ 6 LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
6 LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
6 LþX1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 Lþmin M � L; L� Nf g 6 M
and
SLxðnÞP L�X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj þ
X1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj" #
P L�X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L�X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
P L�min M � L; L� Nf gP N;
which yield that SLðXðN;MÞÞ# XðN;MÞ. Consequently, (2.14) ensures that SL is a contraction mapping and it has a uniquefixed point x 2 XðN;MÞ, that is,
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 569
xðnÞ ¼ LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T ð2:55Þ
and
xðn� sÞ ¼ LþX1i¼1
Xnþð2i�1Þs�1
s¼nþð2i�2Þs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T þ s: ð2:56Þ
Adding (2.55) and (2.56), we have
xðnÞ þ xðn� sÞ ¼ 2LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þsþ
Xnþð2i�1Þs�1
s¼nþ2ði�1Þs
" #
� 1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
¼ 2LþX1s¼n
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
;
n P T þ s:
This together with (2.51) implies that x a bounded nonoscillatory solution of Eq. (1.11). It follow from (2.14), (2.52) and(2.54) that for any m P 0 and n P T ,
xmþ1ðnÞ � xðnÞj ¼ ð1� am � bmÞxmðnÞ þ am LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ hðs; xmðh1ðsÞÞ; xmðh2ðsÞÞ; . . . ; xmðhkðsÞÞÞ½
(������X1t¼s
f ðt; xmðf1ðtÞÞ; xmðf2ðtÞÞ; . . . ; xmðfkðtÞÞÞ þX1t¼s
cðtÞ#)þ bmcmðnÞ � xðnÞ
�����6 ð1� am � bmÞjxmðnÞ � xðnÞj þ amjSLxmðnÞ � SLxðnÞj þ bmjcmðnÞ � xðnÞj6 ð1� am � bmÞkxm � xk þ amhkxm � xk þ 2Mbm 6 ð1� ð1� hÞamÞkxm � xk þ 2Mbm;
which guarantees that (2.7) holds. Thus Lemma 1.1, (2.8) and (2.9) yield that limm!1xm ¼ x.Now we show that (b). In view of (2.21), (2.22) and (2.49), we know that for any distinct L;K 2 ðN;MÞ, there exist h 2 ð0;1Þ
and T > n0 þ sþ jaj satisfying (2.51)–(2.53) and
X1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
<jL� Kj
2M: ð2:57Þ
Let the mapping SL be defined by (2.54), and define a mapping SK : XðN;MÞ ! l1b by (2.54) with L replaced by K. It is clear thatthe mappings SL and SK have the unique fixed points x; y 2 XðN;MÞ, respectively. That is, x and y are bounded nonoscillatorysolutions of Eq. (1.11) in XðN;MÞ. By virtue of (2.54), we deduce that for n P T
xðnÞ ¼ LþX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ hðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ �
X1t¼s
f ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ þX1t¼s
cðtÞ" #
ð2:58Þ
and
yðnÞ ¼ K þX1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞ �
X1t¼s
f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞ þX1t¼s
cðtÞ" #
:
ð2:59Þ
570 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
It follows from (2.2) and (2.57)–(2.59) that for n P T
jxðnÞ � yðnÞjP jL� Kj �X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
P jL� Kj �X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ
�RN;MðsÞmax jxðhlðsÞÞ � yðhlðsÞÞj : 1 6 l 6 kf g
þX1t¼s
PN;MðtÞmax jxðflðtÞÞ � yðflðtÞÞj : 1 6 l 6 kf g#
P jL� Kj �X1i¼1
Xnþ2is�1
s¼nþð2i�1Þs
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
kx� yk
P jL� Kj � 2MX1s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ" #
> 0;
which yields that x – y. This completes the proof. h
Theorem 2.7. Assume that there exists a constant �b 2 0; 12
� �satisfying
jbðnÞj 6 �b; eventually: ð2:60Þ
Let M and N be two positive constants with Mð1� 2�bÞ > N and there exist four mappings PN;M ;QN;M, RN;M;WN;M : Nn0 ! Rþ sat-isfying (2.2), (2.3), (2.21) and (2.22). Then
(a) For any L 2 ðN þ �bM;Mð1� �bÞÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ jaj such that for any x0 2 XðN;MÞ, the Mann iter-ative sequence with errors fxmgmP0 generated by (2.23) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq.(1.11) and satisfies the error estimate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 areany sequences in [0,1] satisfying (2.8) and (2.9);
(b) Eq. (1.11) possesses uncountably bounded nonoscillatory solutions.
Proof. Let L 2 ðN þ �bM;Mð1� �bÞÞ. It follows from (2.21), (2.22) and (2.60) that there exist h 2 ð0;1Þ and T P n0 þ sþ jaj sat-isfying (2.25),
jbðnÞj 6 �b; n P T ð2:61Þ
and
X1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
Q N;MðtÞ þX1t¼s
jcðtÞj" #
6 min Mð1� �bÞ � L; L� �bM � N� �
: ð2:62Þ
Let the mapping SL : XðN;MÞ ! l1b be defined by (2.27). In terms of (2.2), (2.25), (2.27) and (2.61), we gain that forx; y 2 XðN;MÞ and n P T þ 1
jSLxðnÞ � SLyðnÞj 6 jbðnÞjjxðn� sÞ � yðn� sÞj
þXn�1
s¼T
1aðsÞ
�jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞ � hðs; yðh1ðsÞÞ; yðh2ðsÞÞ; . . . ; yðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞ � f ðt; yðf1ðtÞÞ; yðf2ðtÞÞ; . . . ; yðfkðtÞÞÞj#
6�bkx� yk þ
Xn�1
s¼T
1aðsÞ
�RN;MðsÞmax jxðhiðsÞÞ � yðhiðsÞÞj : 1 6 i 6 kf g
þX1t¼s
PN;MðtÞmax jxðfiðtÞÞ � yðfiðtÞÞj : 1 6 i 6 kf g#
6�bþ
Xn�1
s¼T
1aðsÞ RN;MðsÞ þ
X1t¼s
PN;MðtÞ !" #
kx� yk 6 hkx� yk;
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 571
which implies (2.14). It follows from (2.3), (2.27), (2.61) and (2.62) that for any x 2 XðN;MÞ and n P T þ 1
SLxðnÞ 6 Lþ jbðnÞjM þXn�1
s¼T
1aðsÞ
"jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj#
6 Lþ �bM þX1s¼T
1aðsÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
6 Lþ �bM þmin Mð1� �bÞ � L; L� �bM � N� �
6 M
and
SLxðnÞP L� jbðnÞjM �Xn�1
s¼T
1aðsÞ
"jhðs; xðh1ðsÞÞ; xðh2ðsÞÞ; . . . ; xðhkðsÞÞÞj
þX1t¼s
jf ðt; xðf1ðtÞÞ; xðf2ðtÞÞ; . . . ; xðfkðtÞÞÞj þX1t¼s
jcðtÞj#
P L� �bM �X1s¼T
1aðtÞ WN;MðsÞ þ
X1t¼s
QN;MðtÞ þX1t¼s
jcðtÞj" #
P L� �bM �min Mð1� �bÞ � L; L� �bM � N� �
P N;
which imply that SLðXðN;MÞÞ# XðN;MÞ. Consequently, (2.14) means that SL is a contraction mapping and it has a uniquefixed point x 2 XðN;MÞ, which is a bounded nonoscillatory solution of Eq. (1.11). The rest of the proof is similar to that ofTheorem 2.2, and is omitted. This completes the proof. h
Remark 2.1. Theorems 2.1–2.5 extend and improve Theorem 1 in [5].
3. Applications
Now we display seven examples as applications of the results presented in Section 2 and note that Theorem 1 in [5] cannot deal with all these examples.
Example 3.1. Consider the second order nonlinear neutral delay difference equation
D ðnþ 1Þ3D xðnÞ � xðn� sÞð Þ�
þ Dðffiffiffinp
x2ðn3ÞÞ þ ln n
ðnþ 1Þ2x2ðn� 2Þ ¼ ð�1Þn
2n2 þ sin n; n P n0 ¼ 1; ð3:1Þ
where s 2 N is fixed. Let k ¼ 1, M and N be two positive constants with M > N and
aðnÞ ¼ ðnþ 1Þ3; bðnÞ ¼ �1; cðnÞ ¼ ð�1Þn
2n2 þ sin n; f ðn;uÞ ¼ u2 ln n
ðnþ 1Þ2;
hðn;uÞ ¼ffiffiffinp
u2; f 1ðnÞ ¼ n� 2; h1ðnÞ ¼ n3; PN;MðnÞ ¼2M ln n
ðnþ 1Þ2;
Q N;MðnÞ ¼M2 ln n
ðnþ 1Þ2; RN;MðnÞ ¼ 2M
ffiffiffinp
; WN;MðnÞ ¼ M2 ffiffiffinp
; n P 1; u 2 R:
It is easy to verify that the conditions (2.1)–(2.3) are satisfied. Note that
X1n¼n0
naðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
Mn32
ðnþ 1Þ3max 2;Mf g < þ1
and
X1s¼n0
X1t¼s
saðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �¼X1s¼n0
X1t¼s
s
ðsþ 1Þ3max
2M ln t
ðt þ 1Þ2;
M2 ln t
ðt þ 1Þ2;
12t2 þ sin t
( )< þ1:
It follows from Theorem 2.1 that Eq. (3.1) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On the otherhand, for any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ 1 such that the Mann iterative sequence with error fxmgmP0
generated by (2.6) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.1) and has the error estimate (2.7),where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in ½0;1� satisfying (2.8) and (2.9).
572 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
Example 3.2. Consider the second order nonlinear neutral delay difference equation
D n4D xðnÞ þ 2n� 43nþ 2
xðn� sÞ� �� �
þ D ðn2 � 2ffiffiffinp� 4Þxð3n2 � 2Þx2ðn5 � 1Þ
�þ 1
n2 x2 nðn� 1Þðn� 2Þ3
� �x3 nðnþ 1Þ
2
� �
¼ ð�1Þnffiffiffiffiffiffiffiffiffiffiffiffiffiffin5 þ 1p ; n P n0 ¼ 1; ð3:2Þ
where s 2 N is fixed. Let k ¼ 2, �b ¼ 23, M and N be two positive constants with M > N and
aðnÞ ¼ n4; bðnÞ ¼ 2n� 43nþ 2
; cðnÞ ¼ ð�1Þnffiffiffiffiffiffiffiffiffiffiffiffiffiffin5 þ 1p ; f ðn;u; vÞ ¼ u2v3
n2 ;
hðn;u; vÞ ¼ ðn2 � 2ffiffiffinp� 4Þuv2; f 1ðnÞ ¼
nðn� 1Þðn� 2Þ3
; f 2ðnÞ ¼nðnþ 1Þ
2;
h1ðnÞ ¼ 3n2 � 2; h2ðnÞ ¼ n5 � 1; PN;MðnÞ ¼5M4
n2 ; Q N;MðnÞ ¼M5
n2 ;
RN;MðnÞ ¼ 3M2ðn2 þ 2ffiffiffinpþ 4Þ; WN;MðnÞ ¼ M3ðn2 þ 2
ffiffiffinpþ 4Þ; n P 1; u; v 2 R:
It is clear that the conditions (2.2), (2.3) and (2.20) are fulfilled. Note that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
M2
n4 ðn2 þ 2
ffiffiffinpþ 4Þmax 3;Mf g < þ1
and
X1s¼n0X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �¼X1s¼n0
X1t¼s
1s4 max
5M4
t2 ;M5
t2 ;1ffiffiffiffiffiffiffiffiffiffiffiffiffi
t5 þ 1p
( )< þ1:
It follows from Theorem 2.2 that Eq. (3.2) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On the otherhand, for any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ s such that the Mann iterative sequence with error fxmgmP0 gen-erated by (2.23) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.2) and has the error estimate (2.7),where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying (2.8) and (2.9).
Example 3.3. Consider the second order nonlinear neutral delay difference equation
D ðn3 � n2 þ 1ÞD xðnÞ þ 1� n2
1þ 2n2 xðn� sÞ� �� �
þ Dffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
pxðn2 � 2Þ � nx2ðn2 � nÞ
� þ
ffiffiffinp
n2 þ 1x3ðn� 3Þ
� cosðn2 � ln nÞn2 x2ðn3 � 2nÞ
¼ sinðn2 � nÞn2 � nþ 1
; n P n0 ¼ 1; ð3:3Þ
where s 2 N is fixed. Let k ¼ 2, b ¼ � 23, M and N be two positive constants with M > N and
aðnÞ ¼ n3 � n2 þ 1; bðnÞ ¼ 1� n2
1þ 2n2 ; cðnÞ ¼ sinðn2 � nÞn2 � nþ 1
;
f ðn;u; vÞ ¼ffiffiffinp
n2 þ 1u3 � cosðn2 � ln nÞ
n2 v2; hðn; u;vÞ ¼ uffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
p� nv2;
f1ðnÞ ¼ n� 3; f 2ðnÞ ¼ n3 � 2n; h1ðnÞ ¼ n2 � 2; h2ðnÞ ¼ n2 � n;
PN;MðnÞ ¼3M2 ffiffiffi
np
n2 þ 1þ 2M
n2 ; Q N;MðnÞ ¼M3 ffiffiffi
np
n2 þ 1þM2
n2 ;
RN;MðnÞ ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
pþ 2Mn; WN;MðnÞ ¼ M
ffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
pþM2n; n P 1; u;v 2 R:
It is not difficult to verify that the conditions (2.2), (2.3) and (2.31) are fulfilled. Note that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
1n3 � n2 þ 1
maxffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
pþ 2Mn;M
ffiffiffiffiffiffiffiffiffiffiffiffiffiffin2 þ 1
pþM2n
n o< þ1
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �¼X1s¼n0
X1t¼s
1s3 � s2 þ 1
max3M2 ffiffi
tp
t2 þ 1þ 2M
t2 ;M3 ffiffi
tp
t2 þ 1þM2
t2 ;j sinðt2 � tÞj
t2 � t þ 1
( )< þ1:
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 573
Thus Theorem 2.3 ensures that Eq. (3.3) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On the otherhand, for any L 2 N
3 ;M3
�, there exist h 2 ð0;1Þ and T P n0 þ sþ 2 such that the Mann iterative sequence with error
fxmgmP0 generated by (2.23) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.3) and has the error esti-mate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying(2.8) and (2.9).
Example 3.4. Consider the second order nonlinear neutral delay difference equation
D n2D xðnÞ þ 2nþ 3nþ 1
xðn� sÞ� �� �
þ D sinðln nÞx2ðn� 3Þ �
þ 1
nln2nx4ðn� 5Þ ¼ ð�1Þnn
n3 þ 1; n P n0 ¼ 1; ð3:4Þ
where s 2 N is fixed. Let k ¼ 1;a ¼ 1, b ¼ 2; �b ¼ 3, M and N be two positive constants with M > 14N3 and
aðnÞ ¼ n2; bðnÞ ¼ 2nþ 3nþ 1
; cðnÞ ¼ ð�1Þnnn3 þ 1
; f ðn;uÞ ¼ u4
nln2n;
hðn;uÞ ¼ u2 sinðln nÞ; f 1ðnÞ ¼ n� 5; h1ðnÞ ¼ n� 3; PN;M ¼4M3
nln2n;
Q N;MðnÞ ¼M4
nln2n; RN;MðnÞ ¼ 2M; WN;MðnÞ ¼ M2; n P 1; u 2 R:
Obviously, the conditions (2.2), (2.3), (2.35) and (2.36) are satisfied. Note that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
Mn2 max M;2f g < þ1
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �¼X1s¼n0
X1t¼s
1s2 max
4M3
tln2t;
M4
tln2t;
tt3 þ 1
( )< þ1:
Consequently Theorem 2.4 implies that Eq. (3.4) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On theother hand, for any L 2 3N þ 3
2 N;2M þ 23 N
�, there exist h 2 ð0;1Þ and T P n0 þ sþ 4 such that the Mann iterative sequence
with error fxmgmP0 generated by (2.37) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.4) and has theerror estimate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] sat-isfying (2.8) and (2.9).
Example 3.5. Consider the second order nonlinear neutral delay difference equation
D nln2nD xðnÞ � 4nþ ð�1Þnnnþ 1
xðn� sÞ� �� �
þ Dx4ðn� 2Þ
1þ nx2ðn� 2Þ
� �þ x2ðn� 3Þ
n2 þ 1� nx3ðn� 3Þ
n3 þ nþ 1
¼ cosðn�ffiffiffinpþ 1Þffiffiffiffiffiffiffiffiffiffiffiffiffiffi
n3 þ 1p ; n P n0 ¼ 1; ð3:5Þ
where s 2 N is fixed. Let k ¼ 1, b ¼ �5; �b ¼ �2, M and N be two positive constants with M > 4N and
aðnÞ ¼ nln2n; bðnÞ ¼ �4nþ ð�1Þnnnþ 1
; cðnÞ ¼ cosðn�ffiffiffinpþ 1Þffiffiffiffiffiffiffiffiffiffiffiffiffiffi
n3 þ 1p ;
f ðn;uÞ ¼ u2
n2 þ 1� nu3
n3 þ nþ 1; hðn;uÞ ¼ u4
1þ nu2 ; f 1ðnÞ ¼ n� 3; h1ðnÞ ¼ n� 2;
PN;MðnÞ ¼2M
n2 þ 1þ 3M2n
n3 þ nþ 1; QN;MðnÞ ¼
M2
n2 þ 1þ M3n
n3 þ nþ 1;
RN;MðnÞ ¼2M3ð2þM2nÞð1þ N2nÞ2
; WN;MðnÞ ¼M4
1þ N2n; n P 1; u 2 R:
It is clear that the conditions (2.2), (2.3), (2.35) and (2.45) are fulfilled. Note that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
1
nln2nmax
2M3ð2þM2nÞð1þ N2nÞ2
;M4
1þ N2n
( )< þ1
574 Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �
¼X1s¼n0
X1t¼s
1
sln2smax
2Mt2 þ 1
þ 3M2tt3 þ t þ 1
;M2
t2 þ 1þ M3t
t3 þ t þ 1;j cosðt �
ffiffitpþ 1Þjffiffiffiffiffiffiffiffiffiffiffiffiffi
t3 þ 1p
( )< þ1:
Thus Theorem 2.5 yields that Eq. (3.5) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On the otherhand, for any L 2 ð�M;�4NÞ, there exist h 2 ð0;1Þ and T P n0 þ sþ 2 such that the Mann iterative sequence with errorfxmgmP0 generated by (2.37) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.5) and has the error esti-mate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying(2.8) and (2.9).
Example 3.6. Consider the second order nonlinear neutral delay difference equation
D n32D xðnÞ þ xðn� sÞð Þ
� þ D
1� x3ðn3 � 2nþ 1Þnþ x2ðn3 � 2nþ 1Þ
� �þðð�1Þn � 1
nÞx4ðn2 � nÞn2 þ x2ðn2 � nÞ ¼ sin n
nln3n; n P n0 ¼ 1; ð3:6Þ
where s 2 N is fixed. Let k ¼ 1, M and N be two positive constants with M > N and
aðnÞ ¼ n32; bðnÞ ¼ 1; cðnÞ ¼ sin n
nln3n; f ðn;uÞ ¼
ðð�1Þn � 1nÞu4
n2 þ u2 ;
hðn;uÞ ¼ 1� u3
nþ u2 ; f 1ðnÞ ¼ n2 � n; h1ðnÞ ¼ n3 � 2nþ 1;
PN;MðnÞ ¼4M3ðM2 þ 2n2Þðn2 þ N2Þ2
; Q N;MðnÞ ¼2M4
n2 þ N2 ;
RN;MðnÞ ¼Mð2þM3 þ 3MnÞðn2 þ N2Þ2
; WN;MðnÞ ¼1þM3
nþ N2 ; n P 1; u 2 R:
It is clear that the conditions (2.2), (2.3) and (2.49) are fulfilled. Notice that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
1
n32
maxMð2þM3 þ 3MnÞðn2 þ N2Þ2
;1þM3
nþ N2
( )< þ1
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;Q N;MðtÞ; jcðtÞj
� �¼X1s¼n0
X1t¼s
1
s32
max4M3ðM2 þ 2t2Þðt2 þ N2Þ2
;2M4
t2 þ N2 ;j sin tjtln3t
( )< þ1:
Therefore we can invoke Theorem 2.6 to show that Eq. (3.6) possesses uncountably bounded nonoscillatory solutions inXðN;MÞ. On the other hand, for any L 2 ðN;MÞ, there exist h 2 ð0;1Þ and T P n0 þ s such that the Mann iterative sequencewith error fxmgmP0 generated by (2.50) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.6) and hasthe error estimate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in[0,1] satisfying (2.8) and (2.9).
Example 3.7. Consider the following second order nonlinear neutral delay difference equation:
D ðn2 � nþ 2ÞD xðnÞ þ ð�1Þnn3nþ 1
xðn� sÞ� �� �
þ Dnx4ðn2 � 2Þ
n2 þ jxðn2 � 2Þj
� �þð�1Þn�1x5 nðnþ1Þ
2
� nln2nþ x2 nðnþ1Þ
2
�
¼ lnðffiffiffiffiffiffi3npÞ sin n3
n32
; n P n0 ¼ 1; ð3:7Þ
Z. Liu et al. / Applied Mathematics and Computation 213 (2009) 554–576 575
where s 2 N is fixed. Let k ¼ 1, �b ¼ 13, M and N be two positive constants with M > 3N and
aðnÞ ¼ n2 � nþ 2; bðnÞ ¼ ð�1Þnn3nþ 1
Þ; cðnÞ ¼ lnðffiffiffiffiffiffi3npÞ sin n3
n32
;
f ðn;uÞ ¼ ð�1Þn�1u5
nln2nþ u2; hðn; uÞ ¼ nu4
n2 þ juj ; f 1ðnÞ ¼nðnþ 1Þ
2; h1ðnÞ ¼ n2 � 2;
PN;MðnÞ ¼M4ð3M2 þ 5nln2nÞðN2 þ nln2nÞ2
; QN;MðnÞ ¼M5
N2 þ nln2n;
RN;MðnÞ ¼M3nð3M þ 4n2ÞðN þ n2Þ2
; WN;MðnÞ ¼M4n
N þ n2 ; n P 1; u 2 R:
Clearly, the conditions (2.2), (2.3) and (2.60) hold. Notice that
X1n¼n0
1aðnÞ max RN;MðnÞ;WN;MðnÞ
� �¼X1n¼n0
1n2 � nþ 2
maxM3nð3M þ 4n2ÞðN þ n2Þ2
;M4n
N þ n2
( )< þ1
and
X1s¼n0
X1t¼s
1aðsÞ max PN;MðtÞ;QN;MðtÞ; jcðtÞj
� �
¼X1s¼n0
X1t¼s
1s2 � sþ 2
maxM4ð3M2 þ 5tln2tÞðN2 þ tln2tÞ2
;M5
N2 þ tln2t;lnð
ffiffiffiffiffi3tpÞj sin t3jt
32
( )< þ1:
It follows from Theorem 2.7 that Eq. (3.7) possesses uncountably bounded nonoscillatory solutions in XðN;MÞ. On the otherhand, for any L 2 N þ 1
3 M; 23 M
�, there exist h 2 ð0;1Þ and T P n0 þ sþ 2 such that the Mann iterative sequence with error
fxmgmP0 generated by (2.23) converges to a bounded nonoscillatory solution x 2 XðN;MÞ of Eq. (3.7) and has the error esti-mate (2.7), where fcmgmP0 is an arbitrary sequence in XðN;MÞ, famgmP0 and fbmgmP0 are any sequences in [0,1] satisfying(2.8) and (2.9).
Acknowledgements
The authors would like to express their thanks to the anonymous referee for her/his valuable suggestions and comments.This work was supported by the Science Research Foundation of Educational Department of Liaoning Province (2008352)and the Korea Research Foundation Grant funded by the Korean Government (MOEHRD, Basic Research Promotion Fund)(KRF-2008-313-C00042).
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