Hindawi Publishing Corporation The Scientific World Journal Volume 2013, Article ID 640350, 4 pages http://dx.doi.org/10.1155/2013/640350 Research Article A Note on Decomposing a Square Matrix as Sum of Two Square Nilpotent Matrices over an Arbitrary Field Xiaofei Song,1 Baodong Zheng,1 and Chongguang Cao2 1 2 Department of Mathematics, Harbin Institute of Technology, Harbin 150001, China School of Mathematical Sciences, Heilongjiang University, Harbin 150080, China Correspondence should be addressed to Baodong Zheng; [email protected] Received 31 August 2013; Accepted 1 October 2013 Academic Editors: A. Badawi and P. Bracken Copyright © 2013 Xiaofei Song et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Let K be an arbitrary field and X a square matrix over K. Then X is sum of two square nilpotent matrices over K if and only if, for every algebraic extension L of K and arbitrary nonzero πΌ β πΏ, there exist idempotent matrices π1 and π2 over L such that π = πΌπ1 β πΌπ2 . 1. Introduction Botha (see [1]) proved that a square matrix π΄ over a field πΎ is a sum of two nilpotent matrices over πΎ if and only if π΄ is similar to a particular form. In an early paper, Pazzis (see [2]) gave necessary and sufficient conditions in which a matrix can be decomposed as a linear combination of two idempotents with given nonzero coefficients. The goal of this paper is to build a bridge that connects the result obtained in [1] with the result obtained in [2]. However, the relation between these two facts has not been formally discussed yet (more details in [3β9]). If there is no statement, the meanings of notations mentioned in this paragraph hold all over the paper. πΎ denotes an arbitrary field, πΎ is its algebraic closure, πΏ is an arbitrary algebraic extension of πΎ, and car(πΎ) is the characteristic of πΎ. π+ denotes the set of all positive integers, [π ] = {π§ β π+ | 1 β€ π§ β€ π } for some π β π+ . ππ,π (πΎ) denotes the space consisting of all π × π matrices over πΎ; ππ (πΎ) = ππ,π (πΎ). π(π΄) is the rank of π΄ β ππ,π (πΎ). πΈ denotes a vector space over πΎ and dim(πΈ) is the dimension of πΈ. π β ππ (πΎ) is called 2π π in ππ (πΎ) if there exist square nilpotent π1 and π2 β ππ (πΎ) such that π = π1 + π2 , while π is called an (πΌ, π½) composite in ππ (πΎ) if there exist idempotent π1 and π2 β ππ (πΎ) such that π = πΌπ1 + π½π2 , where πΌ, π½ β πΎ \ {0} (Definition 1 in [2]); in particular, π is called ± π if π is an (πΌ, βπΌ) composite in ππ (πΏ) for every algebraic extension πΏ of πΎ and arbitrary nonzero πΌ β πΏ (when car(πΎ) = 2, we still use ± π for the meaning of (πΌ, πΌ) composites). For π β ππ (πΎ), on the one hand, we will prove that π is in ππ (πΎ) implies π is ± π; that is, the form provided by Botha satisfies the condition as in [2]; on the other hand, we will also prove that π is ± π implies π is 2π π in ππ (πΎ); that is, we can derive the form provided in [1] from the results obtained in [2]. In fact, the following theorem is the main result of this paper. 2 π π Theorem 1 (main theorem). Suppose πΎ is an arbitrary field and π β ππ (πΎ); then π is 2π π in ππ (πΎ) if and only if π is ± π. In Section 2, we will state some related theorems and notations from [2] and we will give some necessary corollaries. The proof of Theorem 1 will be carried out in Section 3. 2. More Notations and Necessary Corollaries Suppose π β ππ (πΎ) and ππ β πππ (πΎ), we denote by π = π1 β β β β β ππ the following matrix with βπ π=1 ππ = π: π1 ( π2 d ). (1) ππ Notation 1 (Notation 2 in [2]). Let π β ππ (πΎ), π β πΎ and π β π+ ; we denote by 2 The Scientific World Journal (1) ππ (π, π) the number of blocks of size π for the eigenvalue π in the Jordan reduction of π; (2) ππ (π, π) the number of blocks of size greater or equal to π for the eigenvalue π in the Jordan reduction of π. Definition 2 (Definition 3 in [2]). Two sequences (π’π )π β₯1 and (Vπ )π β₯1 are side to be intertwined if for all π β π+ , Vπ β₯ π’π+1 , and π’π β₯ Vπ+1 . Notation 2 (Notation 4 in [2]). Given a monic polynomial, π = π₯π β ππβ1 π₯πβ1 β β β β β π1 π₯ β π0 , denote the following πΆ(π) by its companion matrix: 0 1 (0 . πΆ (π) = ( ( .. .. . (0 0 β β β β β β 0 0 0 β β β 0 1 0 d 0 π0 π1 π2 ) . ). d d d d .. ) β β β d 1 β β β β β β 0 (2) Corollary 6. Assume car(πΎ) = 2 and let π β ππ (πΎ). Then π is ± π if and only if for every π β πΎ \ {0}, all blocks in the Jordan reduction of π with respect to π have an even size. Naturally, we derive the following corollary from the above two corollaries. Corollary 7. Every nilpotent is ± π. In fact, arbitrary nilpotent is not only ± π but also 2π π. Lemma 8. Every nilpotent π β ππ (πΎ) is 2π π. Proof. For arbitrary field πΎ, let π β ππ (πΎ) is nilpotent; then π is similar to π1 β π2 β β β β β ππ , where for every π β [π ], ππ β πππ (πΎ), βπ π=1 ππ = π, and both the characteristic polynomial and minimal polynomial of ππ are π₯ππ . Furthermore, ππ is similar to πΆ(π₯ππ ) as follows: 0 ππβ2 1 ππβ1 ) 0 0 β β β 1 0 β β β ( .. . d d 0 β β β 1 Theorem 3 (Theorem 1 in [2]). Assume car(πΎ) =ΜΈ 2 and let π β ππ (πΎ). Then π is an (πΌ, βπΌ) composite if and only if all the following conditions hold. (1) The sequences (ππ (π, πΌ))π β₯1 and (ππ (π, βπΌ))π β₯1 are intertwined; (2) for all π β πΎ \ {0, πΌ, βπΌ} and for all π β π+ , ππ (π, π) = ππ (π, βπ). Theorem 4 (Theorem 5 in [2]). Assume car(πΎ) = 2 and let π β ππ (πΎ). Then π is an (πΌ, βπΌ) composite if and only if for every π β πΎ\{0, πΌ}, all blocks in the Jordan reduction of π with respect to π have an even size. Suppose π β ππ (π) is ± π, where car(πΎ) =ΜΈ 2. Then π is (πΌ, βπΌ) composite and (π½, βπ½) composite in ππ (πΏ) for some algebraic extension πΏ of πΎ, where πΌ, π½ β πΏ \ {0} with πΌ =ΜΈ ± π½. By Theorem 3, the following statements are true: (1) for all π β πΎ β {0, πΌ, βπΌ} and for all π β π+ , ππ (π, π) = ππ (π, βπ); (2) for all π β πΎ β {0, π½, βπ½} and for all π β π+ , ππ (π, π) = ππ (π, βπ). so for all π β πΎ\{0} and for all π β π+ , ππ (π, π) = ππ (π, βπ). On the other hand, note that for nonzero πΌ β πΎ with car(πΎ) =ΜΈ 2, the sequences (ππ (π, πΌ))π β₯1 and (ππ (π, βπΌ))π β₯1 are intertwined if for all π β π+ , ππ (π, πΌ) = ππ (π, βπΌ). Then for all π β πΎ \ {0}, π β π+ , ππ (π, π) = ππ (π, βπ) implies that for every algebraic extension πΏ of πΎ and arbitrary nonzero πΌ β πΏ, π is an (πΌ, βπΌ) composite in ππ (πΏ); that is, π is ± π. Therefore the following corollary is true. Corollary 5. Assume car(πΎ) =ΜΈ 2 and let π β ππ (πΎ). Then π is ± π if and only if for all π β πΎ \ {0} for all π β π+ , ππ (π, π) = ππ (π, βπ). Similarly, we can derive the following corollary from Theorem 4. 0 0 .. ) . 0 . (3) ππ ×ππ ππ That is, πΆ(π₯ ) = πΈ2,1 + πΈ3,2 + β β β + πΈππ ,ππ β1 β πππ (πΎ). π /2 π /2β1 π π πΈ2π,2πβ1 + βπ=1 When ππ is even, πΆ(π₯ππ ) = βπ=1 ππ (ππ β1)/2 βπ=1 (ππ β1)/2 βπ=1 πΈ2π+1,2π ; πΈ2π,2πβ1 + πΈ2π+1,2π . when ππ is odd, πΆ(π₯ ) = Note that both β πΈ2π,2πβ1 and β πΈ2π+1,2π are square nilpotent matrices then πΆ(π₯ππ ) is 2π π, and ππ is 2π π follows. Hence π is 2 π π. 3. Proof of Main Theorem 2 π π β ± π. Suppose π β ππ (πΎ) is 2π π in ππ (πΎ); that is, there exist square nilpotent matrices π1 and π2 β ππ (πΎ) such that π = π1 + π2 . It will take two steps to prove π is ± π. Step 1. If π is nonsingular, then π is ± π. Since π = π1 + π2 with π12 = π22 = 0, inspect the eigenspaces of π1 and π2 . Note that π1 and π2 are square nilpotent matrices, their ranks satisfy the following inequality matrices. π (π1 ) + π (π2 ) β€ π, (4) where equality holds if and only if π(π1 ) = π(π2 ) = π/2. At first, π is nonsingular implies 0 is not its eigenvalue. Secondly, if the inequality is strict, then intersection of eigenspaces of π1 and π2 contains nonzero vectors; that is, there exists nonzero π₯ β ππ,1 (πΎ) such that π1 π₯ = π2 π₯ = 0, which implies that 0 is one of eigenvalues of π. This is a contradiction. Hence, π(π1 ) + π(π2 ) = π; that is, π is even and π1 and π2 are similar but not equal. Because π1 is square nilpotent with π(π1 ) = π/2, we can choose π/2 linear independent vectors from the set of its column vectors which can make up a base of eigenspace of π1 and denote π½ by the π × (π/2) matrix consisting of these π/2 columns. Correspondingly, we have π × (π/2) matrix πΎ with The Scientific World Journal 3 all columns from the set of columns of π2 . Because 0 is the only vector in the intersection of eigenspaces of π1 and π2 , π × π matrix (π½ πΎ) is nonsingular. π12 πΎ = 0 implies that nonzero column vectors of π1 πΎ are eigenvectors of π1 and π1 (π½ πΎ) = (0 π1 πΎ) implies π(π1 πΎ) = π/2. Hence; π1 πΎ and π½ are equal under certain column transformation; that is, there is an invertible matrix π1 such that π1 πΎ = π½π1 . Correspondingly, there is an invertible matrix π2 such that π2 π½ = πΎπ2 . π¦ Let ( π¦12 ) be the inverse of (π½ πΎ), where π¦1 and π¦2 are (π/2) × π matrices. Naturally, the following equation is true: 0 πΌ π¦ π½ π¦1 πΎ π¦ ) = ( π/2 π/2 ) . ( 1 ) (π½ πΎ) = ( 1 π¦2 0π/2 πΌπ/2 π¦2 π½ π¦2 πΎ (5) Now, we carry out the same similarity transformation on π1 and π2 as follows: π¦ π π½ π¦1 π1 πΎ π¦ ( 1 ) π1 (π½ πΎ) = ( 1 1 ), π¦2 π¦2 π1 π½ π¦2 π1 πΎ π¦ π π½ π¦1 π2 πΎ π¦ ). ( 1 ) π2 (π½ πΎ) = ( 1 2 π¦2 π¦2 π2 π½ π¦2 π2 πΎ (6) Note that π1 πΎ = π½π1 and π2 π½ = πΎπ2 , the above three 0 π1 ) β ππ (πΎ) and equations imply that π1 is similar to ( 0π/2 π/2 0π/2 π2 is similar to 0 0 ( ππ/22 0π/2 π/2 ) β ππ (πΎ). 0 0 π 0 1 ) + ( ππ/22 0π/2 ). For every Hence, π is similar to ( 0π/2 π/2 0π/2 π/2 algebraic extension πΏ of πΎ and arbitrary nonzero πΌ β πΏ, π is also similar to the following matrix: 0π/2 πΌ πΌβ1 π1 πΌ ) β πΌ ( π/2 ) πΌ ( π/2 0π/2 0π/2 βπΌβ1 π2 0π/2 (7) That is, π is ± π. Step 2. If π is singular and similar to π β π, where π is nonsingular and π is nilpotent. Then π is ± π. At first, we need to prove that π is 2π π. Without loss of generality, we assume π = π β π in the following proof since 2π π holds under similarity transformations. Let π1 = ( ππ13 ππ24 ), where the order of π1 is the same for π and the order of π4 is the same for π. Then π12 = 0 implies the following equations are true: π12 + π2 π3 = 0, π1 π2 + π2 π4 = 0 π3 π1 + π4 π3 = 0, 2 π3 π2 + π42 = 0. (8) π22 = 0, we get the following equations Since (π β π1 ) = after replacing π1 with πβπ1 and π4 with πβπ4 in the previous equations: 2 (π β π1 ) + π2 π3 = 0, (π β π1 ) π2 + π2 (π β π4 ) = 0, π3 (π β π1 ) + (π β π4 ) π3 = 0, 2 π3 π2 + (π β π4 ) = 0. (9) We can derive the following equations from the 3rd and 4th equations in the above two sets of equations: ππ2 + π2 π = 0, π3 π + ππ3 = 0. (10) Note that π is nilpotent, assume its index is π; that is, ππβ1 =ΜΈ 0 and ππ = 0. After multiplying the right side of equation ππ2 + π2 π = 0 by ππβ1 , we can get ππ2 ππβ1 = 0. π is nonsingular implies π2 ππβ1 = 0. Repeat the operation, we eventually get π2 = 0. Similarly, we can also get π3 = 0. So π1 is quasidiagonal and π2 is also quasidiagonal through similar proof; that is, π1 and π4 are square nilpotent same as the corresponding parts of π2 . Finally, we prove that π is 2π π. Since π is ± π by Step 1 and π is ± π by Corollary 7, it is true that π is ± π. 2 ± π β π π. Suppose π β ππ (πΎ) is ± π. If π is similar to πβπ, where π is nonsingular and π is nilpotent, then π is ± π if and only if π is ± π by Corollaries 5, 6, and 7. Without loss of generality, we can assume π is nonsingular. Furthermore, if π is nonsingular and similar to π1 β π2 , where all eigenvalues of π1 are not in πΎ and all eigenvalues of π2 are in πΎ. Then π is ± π if and only if π1 is ± π and π2 is ± π. It will take two steps to prove π is 2π π. Step 3. Suppose car(πΎ) =ΜΈ 2 and all eigenvalues of π are not in πΎ; then for arbitrary nonzero πΌ β πΎ, π is an (πΌ, βπΌ) composite; that is, there exist idempotent matrices π1 and π2 β ππ (πΎ) such that π = πΌπ1 β πΌπ2 . Let π1(0) be the eigenspace of π1 with respect to 0, π(1) 1 the eigenspace of π1 with respect to 1, let π2(0) be the eigenspace of π2 with respect to 0, and π2(1) the eigenspace of π2 with respect to 1. Both πΌ and βπΌ are not eigenvalues of π implies that π1(0) β© π2(0) = π1(1) β© π2(1) = π1(0) β© π2(1) = π1(1) β© π2(0) = {0}; then dim(π1(0) ) = dim(π1(1) ) = dim(π2(0) ) = dim(π2(1) ) = π/2 (otherwise, dim(π1(0) ) β₯ π/2 implies π1(0) β© π2(0) =ΜΈ {0} or π1(0) β© π2(1) =ΜΈ {0}, etc.); that is, π is even. Suppose π and π are π × (π/2) matrices with π(π) = π(π) = π/2 satisfying π1 π = 0 and π2 π = π; then (π π) is π × π nonsingular matrix. Let ( π π ) be its inverse; that is, 0 πΌ π ππ ππ ( ) (π π) = ( ) = ( π/2 π/2 ) . 0π/2 πΌπ/2 π ππ ππ (11) Then we carry out the same similarity transformation on π1 and π2 as follows: ππ1 π 0 ππ π ππ1 π π ( ) π1 (π π) = ( 1 ) = ( π/2 ), 0π/2 ππ1 π ππ1 π ππ1 π π ππ π 0π/2 ππ π ππ2 π π ), )=( 2 ( ) π2 (π π) = ( 2 ππ2 π πΌπ/2 ππ2 π ππ2 π π (12) where π1 and π2 are idempotent implies that ππ1 π and ππ2 π are idempotent and π(π1 ) = π(π2 ) = π/2 implies that ππ1 π = πΌπ/2 and ππ2 π = 0π/2 . Hence, π is similar to the following matrix: 0 0 πΌππ1 π 0π/2 ) + ( π/2 ). (13) ( π/2 0π/2 0π/2 βπΌππ2 π 0π/2 That is, π is 2π π in ππ (πΎ). 4 The Scientific World Journal When car(πΎ) = 2, π is (πΌ, πΌ) composite for arbitrary nonzero πΌ β πΎ, we can similarly prove that π is 2π π in ππ (πΎ) replacing βπΌ with πΌ in the previous proof. Step 4. Suppose car(πΎ) =ΜΈ 2 and all eigenvalues of π are in πΎ; then by Corollary 5, ππ (π, πΌ) = ππ (π, βπΌ) for every π β π+ and arbitrary nonzero πΌ β πΎ. Moreover, π is similar to π1 β β β β β ππ , where both the characteristic polynomial and the minimal polynomial of ππ are [(π₯ β πΌπ )(π₯ + πΌπ )]ππ = (π₯2 β πΌπ2 )ππ with 2 βπ π=1 ππ = π and πΌπ β πΎ\{0} is one of eigenvalues of π for every π β [π ]. Without loss of generality, we just need to prove ππ is 2π π. Since ππ is similar to πΆ((π₯2 β πΌπ2 )ππ ) as follows: 0 1 0 ( ( .. (. .. . 0 ( 0 β β β β β β 0 0 β β β β β β 0 1 0 β β β 0 . d d d .. π0 0 π2 ) .. ) , . ) (14) d d 1 0 π2ππ β2 β β β β β β 0 1 0 ) where (π₯2 β πΌπ2 )ππ = π₯2ππ β π2ππ β2 π₯2ππ β2 β β β β β π2 π₯2 β π0 . We have πΆ((π₯2 β πΌπ2 )ππ ) = πΈ2,1 + β β β + πΈ2ππ ,2ππ β1 + π0 πΈ1,2ππ + π2 πΈ3,2ππ + β β β + π2ππ β2 πΈ2ππ β1,2ππ = (πΈ2,1 + πΈ4,3 + β β β + πΈ2ππ ,2ππ β1 ) + (πΈ3,2 + β β β + πΈ2ππ β1,2ππ β2 + π0 πΈ1,2ππ + π2 πΈ3,2ππ + β β β + π2ππ β2 πΈ2ππ β1,2ππ ) = π1 + π2 . Obviously, both π1 and π2 are square nilpotent matrices; that is, ππ is 2π π. Hence, π is 2π π in ππ (πΎ). When car(πΎ) = 2, all blocks in the Jordan reduction of π with respect to πΌ β πΎ \ {0} have an even size by Corollary 6; that is, both the characteristic polynomial and minimal polynomial of every block with respect to πΌ are (π₯ + πΌ)π π = ((π₯ + πΌ)2 )π π /2 = (π₯2 + πΌ2 )π π /2 , where π π is even. Similarly, we can also prove that π is 2π π in ππ (πΎ). References [1] J. D. Botha, βSums of two square-zero matrices over an arbitrary field,β Linear Algebra and Its Applications, vol. 436, no. 3, pp. 516β524, 2012. [2] C. D. Pazzis, βOn linear combinations of two idempotent matrices over an arbitrary field,β Linear Algebra and Its Applications, vol. 433, no. 3, pp. 625β636, 2010. [3] R. E. Hartwig and M. S. Putcha, βWhen is a matrix a difference of two idempotents?β Linear and Multilinear Algebra, vol. 26, no. 4, pp. 267β277, 1990. [4] J. H. Wang and P. Y. Wu, βSums of square-zero operators,β Studia Mathematica, vol. 99, no. 2, pp. 115β127, 1991. [5] F. R. 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