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JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mat hematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space of k-Commutative Matrices l Marvin Marcus 2 and N. A. Khan 3 (A ugu st 14, 1959) L et [A, X J= AX - XA a nd [A, Xh =[A, [A, Xh-d. Those matrices X which "k-co m- mu te " with a fix ed m at rix A are in vest igat ed. In particular, the dimension of the null sp ac e of the lin ea r tr an sformat ion T(X) = [A., Xh when A is non der ogatory is de te rm in ed. 1. Introduction Let A be a :fix ed N -s quar e complex matrix and let [A, Xl= AX- XA, [A, Xh=[A, [ A, Xh-ll. It is easil y checked th at It is clear t ha t the set of X such t ha t [A , Xh =O is a linear subspace of the spa ce MN of all N -square complex matri ces. This subspace is denoted by Qk (A ). In theor em 1 is determin ed t h e dim ension of Qk( A) in terms of the degrees of th e elem en t ary divisors of A wh en th ere is ex actly one cleme ntary divisor for each eige nv alue. Let Eq deno te the set of matri ces in MN with pr ec isely q di stin ct eigen- values. In th eorem 2 it is shown th at in case then min dim Qk(A) = R(Q+ 1) 2+ (q- R)Q2 A,E, nM N wher eN= Qq +R, O-:;' R< q. Th e maximum is also found. 2 . Results L et T d en ote the lin ear transform at ion on MN de- fined by T (A) = [A , Xl and we note th at T k( X) = [ A, Xh- Wi th r es p ect to the ba sis E ij in M N, or- dered l exicographi cally, we check th at T has the m atrix representation IN®A - A'® I N' Th e n ot a- tion is th e following : Eij is the N-s qu are m at rix with 1 in position i, j, 0 elsewhere; I N®A denotes the Kr on eck er product of the N-square identi ty IN with A. It is clear t ha t one m ay ass um e A is in Jordan canonical form q J s, (2 .1 ) 8= 1 where indicates dir ect s um and the J s ar e the Jord an blocks corr espondin g to the di stin ct eigen- 1 This work was supported in part by U.S. ational Science Foundation Gr ant NSFG- 541 6. I Present address: The UniverSity of British Columbia, Vancouver, Canada. Present address: Muslim University, Aligarh, India. 51 valu es As, 8= 1, ... , q, of A. If T k(A) =O and X is partitioned conformally with the par titioning (2.1 ) of A, Roth 4 shows t ha t q X= ,2: · X s' 8= 1 where Xs is th e same siz e as J s, 8= 1, . . . , q. If , fur ther, each J s is decomposed into a dir ect sum of companion ma tri ces of the elem en ta ry divisors cor- responding to As one m ay also eff ect a conformal pa rtitioning of the corr es ponding A s. It is also clear that one may ta ke A s= O in examining th e st ruct ur e of Xs since [J ., X ,h remains invari ant up on t ran sla- tion of J s• W ea re t hus redu ced to co nsidering the fo llowing sit ua tion in determinin g the dimension of Qk (A ): Let where U rt is an ri-s quare auxiliary uni t m at rix, an unbr oken line of l 's along the fir st super-di agonal O 's elsewhere, and suppose [U , Yh = O. Partition Y conformally with U , Y = (Yij) i, j = 1, . . . , l where Y tj is rt X r" a nd by (1.1 ) i ,j = l , . . . ,l (2.2 ) is equi valen t to [U, Yh= O. Th e problem th en is to d etermin e the numb er of arbit rar y pa ram eters in each Y tj . Equ at ion (2.2) for a :fixed i, j represents a linear transformation mappin g Y ij into 0, a nd with respect to a suitably chosen basis this transform at ion has the m atrix represen tat ion wh er e (2 .3) To simplify th e no tat ion, put rt=n, rj = m wh ere it can be a ss umed wit hou t loss of generality t ha t n m. The similari ty invarian ts of T ij as compu te d by , W. E. Rot h, On k-commutative matrices, Tr aus. Am. M at h. Soc. 3 9 483 '

Space of k-commutative matrices - NIST...JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space

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Page 1: Space of k-commutative matrices - NIST...JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space

JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960

Space of k-Commutative Matrices l

Marvin Marcus 2 and N. A. Khan 3

(A ugust 14, 1959)

Let [A, X J= AX- XA and [A, Xh = [A, [A , Xh- d. Those m at rices X which "k-com­mute" wit h a fixed m atrix A are invest igated . In pa r t icular, t he dimens ion of the null space of t he linear t ransformation T (X ) = [A., Xh wh en A is non derogatory is dete rmin ed.

1. Introduction

Let A be a :fixed N -square complex matrix and let [A , X l = A X - X A , [A, X h = [A, [A, Xh-ll . It is easily checked that

It is clear that the se t of X such tha t [A , Xh= O is a linear subspace of the space M N of all N -square complex matrices. This subspace is deno ted by Qk(A) . In theorem 1 is determined t he dimension of Qk(A ) in terms of the degrees of the elem en tary divisors of A when there is exactly one clementary divisor for each eigenvalue. Let Eq denote the set of matrices in M N with precisely q distinct eigen­values. In theorem 2 it is shown that in case k ~ 2 (N- q) + 1 , then

min dim Qk(A) = R(Q+ 1) 2+ (q- R)Q2 A,E,nM N

whereN= Qq + R , O-:;' R< q. The maximum is also found .

2 . Results

Let T denote the linear transformation on MN de­fined by T(A) = [A , Xl and we no te that T k(X) = [A, Xh- With respect to the basis E ij in M N , or­dered lexicographically , we ch eck that T has the matrix represen tat ion I N®A - A'® I N' The n ota­tion is the following : E i j is the N-square matrix with 1 in position i, j, 0 elsewhere; IN®A denotes the Kron ecker product of the N -square iden tity matrL~ I N with A. It is clear tha t one may assume A is in Jordan canonical form

q • A=~ J s, (2 .1)

8= 1

where ~. indicates direct sum and the J s are the Jordan blocks corresponding to the distinct eigen-

1 T his work was supported in part by U.S. ational Science Foundation Grant NSFG- 5416.

I Present address: T he UniverSity of British Colum bia, Vancouver, Canada. • Present address: Muslim University, Aligarh, India.

51

values As, 8= 1, ... , q, of A . If Tk(A) = O and X is partitioned conformally with the parti tioning (2.1 ) of A , Ro th 4 shows that

q

X = ,2: · X s' 8= 1

where X s is the same size as J s, 8= 1, . . . , q. If, fur ther , each J s is decomposed into a direct sum of companion matrices of the elem entary divisors cor ­responding to As one may also effect a conformal partitioning of the corresponding A s. It is also clear that one may tak e As= O in examining the structure of X s since [J ., X ,h remains invarian t upon transla­tion of J s• Weare thus reduced to considering the following si tua tion in determining the dimension of Qk(A) : Let

where Urt is an r i-squar e auxiliary unit m atrix, an unbroken line of l 's along the first super-diagon al O's elsewhere, and suppose [U , Yh= O. Par tition Y conformally with U, Y = (Yij ) i , j = 1, . . . , l where Y t j is rt X r" and by (1.1 )

i ,j= l , . . . , l

(2.2)

is equivalen t to [U, Yh = O. The problem th en is to determine the number of arbitrary parameters in each Y tj .

Equation (2.2) for a :fixed i , j represen ts a linear transforma tion mapping Y ij into 0, and wi th respec t to a suitably chosen basis this transformation has the matrix represen tation Tt~ where

(2 .3)

T o simplify the no tation, put rt= n , rj= m where it can be assumed without loss of gen erality that n ~ m. The similarity invar ian ts of T ij as computed by

, W. E. Roth, On k-commutative matrices, Traus. Am. M ath. Soc. 3 9 483 ~0. '

Page 2: Space of k-commutative matrices - NIST...JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space

Ro th 5 are flex) = . .. = fmn - m(x) = 1, fmn-m+v(X) = xll.+2v- I, p=l, ... , m and fl = n-m. H ence T ij is similar to the direct sum of the companion matrices of these nontrivial similarity invariants,

m Tij G;t,. 2,2 · 0(XIl.+ 2V - I). (2.4)

p = 1

The sizes of these companion matrices arranged in decreasing order are fl + 2m- 1, fl + 2m-3, ... , fl + 3, fl + 1.

Now, if k ?: fl + 2p- 1, then (O(x t.+2v- 1))k= O. If k < fl + 2p- 1, then

p( {C(XIl.+ 2p - l) }k) = fl + 2p - 1- k,

where p denotes rank. Let TJ denote nullity.

L E MMA 1: (a)

(b)

(e)

ij l~k<fl,

TJ(T~j) =km- (k -; fly +0

ij fl~k<m+n- 1,

TJ(T7j)= mn ij k?: m + n - 1,

where Cis 0 01' 1/4 according as (k - fl ) is even 01' odd.

PROOF:

(a)

Then m

p(T~j) = 2,2 (fl + 2p- 1- k) = mn-mk, p = 1

and

(b) fl ~k<n+m- l.

Assume k - fl is odd and observe that the size of the (m - (k- fl + l ) /2) th companion m atrix: in (2.4) IS

fl + 2m- ( 2( m (k-~+ l ) )_ l ) = k+ 2,

and the size of the next companion matrix IS k. H ence,

p (Ttj) = (fl + 2m-1 - k) + (fl + 2m- 3- k) + . ..

+ (k+ 2- k).

The last term in this sum is the rank of the kth power of the (m-(k- fl + l) /2) th companion matrL,(

in (2.4) . Thus,

P(T;i) = (2m - k:fl - 1)em - k: fl + 1)

=( m - (k-; fl)Y-l In case k - fl is even , it is observed that the size of the (m-(k - fl )/2)th companion matrix in (2.4) is k + 1. Also the size of the n ext companion matrix is k-l. H ence,

p(T~j) = (fl + 2m-1 - k) + (fl + 2m - 3- 1C) + .. . + (k+ 1- k)

Hence, in either case

TJ(Ti~) =mn-p(Ti~)

= mn-( m- (k-;fl)Y + 0

( k- fl)2 = mk- - 2- +0

where 0 is 0 or 1/4 depending on whether k- fl lS

even or odd.

(c) lc?:m + n- l.

Then

and

THEOREM 1. Assume A is N -square with distinct eigenvalues AI , . .. , Aq and let (x - Aj)'; be the elemen­tary divisors oj A, j = l , .. . , q, €1 ?: €22: .. . ?: €q. Partition the integers 1, . . . , q so that

Then

(i) dim Qk(A) = kN-q (~-O) if k< 2€q- 1,

' W. E. Roth , On direct product matriccs, Bull . Am . M ath. Soc. 40, 461 (1934). 0 01' X according as k is even 01' odd.

52

Page 3: Space of k-commutative matrices - NIST...JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space

PROOF: Since there is only one elementary divisor of A for each eigenvalu e of A it may be assumed, as in (2.1) , that

where J s= )...1" + U." unit matrix s= 1 in Qk(A), , ,

U" the Es-Sq uare auxiliary ., q. Then, if X is contained

q

X = "" · X £...J Sl 8=1

where X s is E,-square, s= I , . . . , q. By lemma 1 we know that the number of arbitrary parameters in X s is (by putting m = n = Es)

(b)

(c)

p n,= Esk--4+ C

Consider (i) first: lc < 2Eq- 1. Then lc < 2Eqj-l j = I , ... , l, and hence X s has n s arbitrary pat·am­eters in it. There are qu- qU- l values of s such that n ,=n q• (qo = O for convenience) . Hence,

p In this case nq. = Et, (1 = t, . .. , land 'nqu = lcEqu -4+ 0 ,

(1 = 1, ... , t-I. H ence,

/-1 I

dim Qk(A) = ~ (q. - q' - l)nqu + ~ (q. - qU- l) Et u-l u= t

If (iii) k2::2El-l, thenk2::2Ej-l forj = l , ... , q and

q

dim Q..,(A) = 2:E;. 8= 1

632245- 60- 5 53

In case there is more than one elementary divisor corresponding to a particular eigenvalue there does not seem to be any simple formula for dim Qk(A) in terms of the degrees of the elementary divisors of A. However, by repeated use of lemma 1, it is pos­sible to compute dim Qk(A) for any par t icular A. For example, if

A =

2

o

o

o

1

2

o

o

o

1

2

o 2

then dim Qk(A) = 37 for k = 3.

N ext are determin ed the largest and smallest values that dim Qk(A) may take on as A varies over Eq , the set of matrices with precisely q distinct eigenvalues, under the condi tion that lc 2::2(N-q) + 1.

L EMMA 2. I f El 2:: . . . 2:: Eu are positive integers satisfying

O~R< q,

then

The lower bound i s achievedjol'

El = ... = En= Q+ l , En+,= . . . = Eq= Q,

and the uIper bound i s achieved jur

El = N - q+ l and E2= ... = Eq= I.

PROOF. The lower inequality is proved by induc­tion on R. In case R = O, then N /q= Q, and if El, .. . , Eq are regarded as continuous variables, then

± dhasaminimumfoI"Ej= Q, j = I , . .. , q. Now j= ]

suppose the result is true for aU remainders obtained by dividing N by q that are less than R. We first claim that there exists an in teger i< q such that Ej> EHI and Ei2::Q + l. Clearly the setoI in tegersj such that E j 2:: Q+ 1 is nonempty otherwise (since R > O),

Let i be the largest integer j such that Ej 2:: Q+ 1 ; then if i were q, El2:: .. . 2:: Eq 2:: Q+ 1 and

Page 4: Space of k-commutative matrices - NIST...JOURNAL OF RESEARCH of the National Bureau of Standards- B. Mathematics and Mathematical Physics Vol. 64B, No. 1. January-March 1960 Space

Hence i < q and from the definition of i, €i> €i+l' Let }lj= €iJ j ~ i and }li= €i- l. Then J1.1'2. . '2. J1. q, }ll+' " + J1. q= N - 1= Qq + R - 1, and by induction

and thus, q

~€~'2. R(Q+ 1)2+ (q-R) Q2+2(€i- Q- 1). j=l

Since €i'2.Q+1, the proof is complete. The upper bound is easily obtained.

THEOREM 2. If k '2. 2 (N-q) + I , then

min dim Gk (A) = R (Q+ 1)2+(q- R)Q2 A.E,nMN

and max dim Gk(A) = (N - q+ 1)2+q- 1, A.E ,nlofN

where N qQ+ R ,

54

PROOF. Let AeEq and suppose el '2. . . . '2. €q are such integers that e j is the sum of the degrees of all elementary divisors of A corresponding to A.iJ j = l, ... , q.

Then

and hence, €1~N- q+ 1 and 2€1 - 1~k. Thus lc is at least 2}l - 1 where J1. is the degree of any elemen­tary divisor of A. From lemma lone may check in this case that min dim Gk(A ) may be evaluated

A.E.nMN

by confming A to those matrices having precisel~r one elementary divisor for each eigenvalue. Hence (x- A. j) €j may be taken as the elementary divisors of A, j = l, . . . , q. By theorem 1 if AeEq,

and the results follow from lemma 2.

WASHING'l'ON, D.C. (Paper 64Bl- 21 )