Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 247028, 10 pages http://dx.doi.org/10.1155/2013/247028 Research Article New Representations of the Group Inverse of 2 × 2 Block Matrices Xiaoji Liu, Qi Yang, and Hongwei Jin College of Science, Guangxi University for Nationalities, Nanning 530006, China Correspondence should be addressed to Xiaoji Liu; xiaojiliu72@126.com Received 13 March 2013; Accepted 25 June 2013 Academic Editor: Mehmet Sezer Copyright © 2013 Xiaoji Liu 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. This paper presents a full rank factorization of a 2 × 2 block matrix without any restriction concerning the group inverse. Applying this factorization, we obtain an explicit representation of the group inverse in terms of four individual blocks of the partitioned matrix without certain restriction. We also derive some important coincidence theorems, including the expressions of the group inverse with Banachiewicz-Schur forms. 1. Introduction Let Cπ×π denote the set of all π × π complex matrices. We use π (π΄), π(π΄), and π(π΄) to denote the range, the null space, and the rank of a matrix π΄, respectively. The Moore-Penrose inverse of a matrix π΄ ∈ Cπ×π is a matrix π ∈ Cπ×π which satisfies (1) π΄ππ΄ = π΄ ∗ (3) (π΄π) = π΄π (2) ππ΄π = π ∗ (4) (ππ΄) = ππ΄. (1) The Moore-Penrose inverse of π΄ is unique, and it is denoted by 𴆠. Recall that the group inverse of π΄ is the unique matrix π ∈ Cπ×π satisfying π΄ππ΄ = π΄, ππ΄π = π, π΄π = ππ΄. (2) The matrix π is called the group inverse of π΄ and it is denoted by π΄# . Partitioned matrices are very useful in investigating various properties of generalized inverses and hence can be widely used in the matrix theory and have many other applications (see [1–4]). There are various useful ways to write a matrix as the product of two or three other matrices that have special properties. For example, linear algebra texts relate Gaussian elimination to the LU factorization and the Gram-Schmidt process to the QR factorization. In this paper, we consider a factorization based on the full rank factorization of a matrix. Our purpose is to provide an integrated theoretical development of and setting for understanding a number of topics in linear algebra, such as the Moore-Penrose inverse and the group inverse. A full rank factorization of π΄ is in the form π΄ = πΉπ΄ πΊπ΄ , (3) where πΉπ΄ is of full column rank and πΊπ΄ is of full row rank. Any choice in (3) is acceptable throughout the paper, although this factorization is not unique. For a complex matrix A of the form A=[ π΄ π΅ ] ∈ C(π+π )×(π+π‘) , πΆ π· (4) in the case when π = π and π΄ is invertible, the Schur complement of π΄ in A is defined by π = π· − πΆπ΄−1 π΅. Sometimes, we denote the Schur complement of π΄ in A by (A/π΄). Similarly, if π = π‘ and π· is invertible, then the Schur complement of π· in A is defined by π = π΄ − π΅π·−1 πΆ. In the case when π΄ is not invertible, the generalized Schur complement of π΄ in A is defined by π = π· − πΆπ΄† π΅. (5) Similarly, the generalized Schur complement of π· in A is defined by π = π΄ − π΅π·† πΆ. (6) 2 Journal of Applied Mathematics The Schur complement and generalized Schur complement have quite important applications in the matrix theory, statistics, numerical analysis, applied mathematics, and so forth. There are a great deal of works [5–8] for the representations of the generalized inverse of A. Various other generalized inverses have also been researched by a lot of researchers, for example, Burns et al. [6], Marsaglia and Styan [8], BenΔ±Μtez and Thome [9], CvetkovicΜ-IlicΜ et al. [10], Miao [11], Chen et al., and so forth [12] and the references therein. The concept of a group inverse has numerous applications in matrix theory, from convergence to Markov chains and from generalized inverses to matrix equations. Furthermore, the group inverse of block matrix has many applications in singular differential equations, Markov chains iterative methods, and so forth [13–17]. Some results for the group inverse of a 2 × 2 block matrix (operator) can be found in [18– 30]. Most works in the literature concerning representations for the group inverses of partitioned matrices were carried out under certain restrictions on their blocks. Very recently, Yan [31] obtained an explicit representation of the Moore-Penrose inverse in terms of four individual blocks of the partitioned matrix by using the full rank factorization without any restriction. This motivates us to investigate the representations of the group inverse without certain restrictions. In this paper, we aimed at a new method in giving the representation of the group inverse for the fact that there is no known representation for A# , Aπ· with π΄, π΅, πΆ, and π· arbitrarily. The outline of our paper is as follows. In Section 2, we first present a full rank factorization of A using previous results by Marsaglia and Styan [8]. Inspired by this factorization, we extend the analysis to obtain an explicit representation of the group inverse of A without any restriction. Furthermore, we discuss variants special forms with the corresponding consequences, including Banachiewicz-Schur forms and some other extensions as well. Yan [31] initially considered the representation of the MoorePenrose inverse of the partitioned matrix by using the full rank factorization technique. The following result is borrowed from [31, Theorem 2.2]. For convenience, we first state some notations which will be helpful throughout the paper: ππΌ = πΌ − πΌ− πΌ, † π = π· − πΆπ΄ π΅, π = πΆππ΄ , where πΌ− ∈ πΌ {1} , πΈ = ππ΄π΅, π = πππππΈ . (7) (8) π = πΉππΊπ, πΈ = πΉπΈ πΊπΈ , π = πΉπ πΊπ , A = πΉπΊ = [ † πΆπΊπ΄ πΉπ΄† π΅ ] πΊπ ] ] ]. † ] πΉππ] πΊπΈ ] (10) Now, the Moore-Penrose inverse of A can be expressed as A† = πΊ† πΉ† . In particular, when π΄ is group inverse, let π = π· − πΆπ΄# π΅; then the full rank factorization of A is πΉπ΄ A=[ # πΆπ΄ πΉπ΄ πΊπ΄ πΊπ΄ π΄# π΅ ] [ 0 0 πΉπΈ πΊπ ] [ 0 ]. [ ] ] † πΉπ πΉπ ππππΊπΈ† [ π ] [πΊπ πΉπ [ 0 (11) πΊπΈ ] This motivates us to obtain some new results concerning the group inverse by using the full rank factorization related to the group inverse. Recall that if a matrix π΄ ∈ Cπ×π is group inverse (which is true when ind(π΄) = 1), then π΄# can be expressed in terms of π΄{1}; that is, 3 π΄# = π΄(π΄(1) ) π΄. (12) Particularly, we have 3 π΄# = π΄ (𴆠) π΄. (13) Theorem 1. Let A be defined by (4); then the group inverse of A can be expressed as A# = [ π΄ π΅ ] πΆ π· × [(π5 + π5 π3 π2∗ π1 π2 − π4 π1 π2 ) π3 π† 0 ×[ ] (π3 π5 + π2∗ π1 π2 π5 − π2∗ π1 π4 ) 0 πΈ† + (π4 − π5 π3 π2∗ ) π1 [ Let π΄, πΈ, π, π have the full rank factorizations π΄ = πΉπ΄ πΊπ΄, πΉπ΄ πΊπ΄ [ [ 0 0 0 πΉπΈ [ ] † [ πΉπ πΉπ ππππΊπΈ [ [πΊπ [ 0 The following result follows by using [31, Theorem 3.6] and (13). 2. Representation of the Group Inverse: General Case ππΌ = πΌ − πΌπΌ− , respectively; then there is a full rank factorization of the block matrix A: 3 (9) 𴆠0 ] 0 π † × π1 (π4 − π2 π5 )] [ π΄ π΅ ], πΆ π· (14) Journal of Applied Mathematics 3 † + (π4 − π5 π3 π2∗ ) π1 [π΄ 0† ] 0 π where πΉ1 = [ πΊ1 = [ π1 = [ † πΊπ΄ 0 πΉπ΄† 0 ], 0 πΉπ † ∗ πΉ2 = [ 0 ∗] , πΊπ † † 0 πΉπ ], 0 πΉπΈ† πΊ2 = [ π3−1 † πΊπ 0 ∗ 3 π΄ π΅ × π1 (π4 − π2 π5 )] [πΆ π·] , 0 ∗] , πΊπΈ† −π3−1 π»ππ π2−1 π4 −π4∗ π2−1 ππ π»∗ π3−1 π4 + π4∗ π2−1 ππ π»∗ π3−1 π»ππ π2−1 π4 π2 = [ π»πππ»1∗ π1−1 ], πππ»1∗ π1−1 π» πΌ π4 = [ π1 = [ πΌ π» ], 0 πΌ π3−1 π3 = [ πΉ† = [ πΉ1 π1 π4 − πΉ1 π1 π2 π5 ], −πΉ2 π∗ π1 π4 + πΉ2 (π3 + π2∗ π1 π2 ) π5 πΊ† = ], ∗ π»=π΄ πΆ , π4 = [ (a) If πΈ is of full column rank and π is of full row rank, then π΄ π΅ A# = [ ] πΆ π· πΌ 0 ], πΎ∗ πΌ π† π 0 ], πΎ1∗ πΈ† πΈ (15) × ([ π»1 = πΈ π , ×[ πΎ = π΄ π΅, π2 = πΌ + † π4 = (π π † π2−1 π π † ) , A# = [ ×[ † π4 = (π † π π2−1 π † π ) . If the (1, 1)-element π΄ of A is group inverse, we immediately have Theorem 2 by using the full rank factorization of (11). Theorem 2. Let A be defined by (4). Suppose π΄ is group inverse; then the group inverse of A can be expressed as π΄ π΅ ] πΆ π· × [(π5 + ×[ − π4 π1 π2 ) π3 π† 0 ] (π3 π5 + π2∗ π1 π2 π5 − π2∗ π1 π4 ) 0 πΈ† Μ Μ π −ππΎ 𴆠0 ] ∗Μ ∗Μ ][ 0 π† ππ πΎ π πΌ − ππ πΎ ππΎ 3 Μ Μ π π ππ»π ×[ ∗ ]) Μ πΌ − π»∗ ππ»π Μ π −π» π π2 = πΌ + ππΈ πΎ1∗ πΎ1 ππΈ , π5 π3 π2∗ π1 π2 3 π΄ π΅ −π»∗ πΌ ]) [ ]. πΌ 0 πΆ π· π΄ π΅ ] πΆ π· × ([ (16) π3 = πΌ + πΎππΈ (π2−1 − π2−1 π4 π2−1 ) ππΈ πΎ∗ , A# = [ (20) (b) If πΈ = 0, π = 0, then πππ»1∗ π»1 ππ, π3 = πΌ + π»ππ (π2−1 − π2−1 π4 π2−1 ) πππ»∗ , π1 = πΌ + πΎ1 ππΈ πΎ1∗ , πΌ −πΎ − πΎ1 π† 0 𴆠0 ] ][ ]+[ 0 πΌ 0 0 0 πΈ† † πΎ1 = π† π, π1 = πΌ + (19) Theorem 3. Let A be defined by (4); then the following statements are true. †∗ ∗ π»1 πππ»1∗ , (18) will be helpful in the proofs of the following results. with †∗ −π4 π1 π2 π3 πΊ2∗ + π5 (π3 + π3 π2∗ π1 π2 π3 ) πΊ2∗ ] , [π4 π1 πΊ1∗ − π5 π3 π2∗ π1 πΊ1∗ , πΎ ], 0 −π1−1 πΎ1 π1−1 ], ∗ −1 −πΎ1 π1 πΌ + πΎ1∗ π1−1 πΎ1 π5 = [ The two representations of πΉ† , πΊ† (which can be found in [31, Theorem 3.1]), 0 ππ ], πΈπΈ† π»1 ππ −π4 π2−1 ππΈ πΎ∗ π3−1 π4 + π4 π2−1 ππΈ πΎ∗ π3−1 πΎππΈ π2−1 π4 πΎπΎ∗ [ ∗1 πΎ1 where π» = π΄ πΆ∗ , πΎ = π΄# π΅, and π»1 , πΎ1 , π1 , π2 , π3 , π4 , π5 , π1 , π2 , π3 , π4 , π5 , π1 , π2 , π3 , π4 , π1 , π2 , π3 , π4 are the same as those in Theorem 1. † −π3−1 πΎππΈ π2−1 π4 π2 = ], πΌ 0 π3 = [ ], 0 π1−1 π5 = [ (17) #∗ (21) π΄ π΅ ], πΆ π· Μ = (πΌ + πΎππ πΎ∗ )−1 . Μ = (πΌ + π»ππ π»∗ )−1 and π where π Proof. (a) If πΈ is full row rank, then ππΈ = 0, and hence π = 0, π1 = πΌ, π2 = πΌ, π3 = πΌ, and π4 = 0. Thus, π1 , π2 , π3 , π4 , π5 defined in Theorem 1 can be simplified to π1 = [ π3 = [ πΌ 0 ], 0 0 π2 = [ πΌ −πΎ1 ], ∗ −πΎ1 πΌ + πΎ1∗ πΎ1 π5 = [ πΎπΎ1∗ πΎ ], πΎ1∗ 0 πΌ 0 π4 = [ ∗ ] , πΎ πΌ π† π 0 ], πΎ1∗ πΌ (22) 4 Journal of Applied Mathematics (b) If πΈ = 0, then π»1 = 0, π1 = πΌ, and π2 = πΌ such that π3 = πΌ+π»ππππ πππ»∗ and π4 = π π † . Letting π = π3−1 , then which imply πΌ 0 π4 π1 = [ ∗ ] , πΎ 0 π2 π3 = [ π1 π2 π3 = [ π5 π3 π2∗ π1 π5 π3 = [ 0 0 = [ ∗ ], πΎ 0 0 πΎ ], πΎ1∗ −πΎ1∗ πΎ π1 = [ 0 πΎ ], 0 0 π» 0 π2 = [ ], πΌ 0 0 πΎ π4 π1 π2 π3 = [ ], 0 πΎ∗ πΎ † π π −πΎ1 ], 0 πΌ π5 π3 π2∗ π1 π2 π3 = [ 0 0 ]. 0 πΎ∗ πΎ (23) π4 = [ 0 0 πΌ πΌ −πΎ − πΎ1 [ † ] 0 πΊπ 0 ]. 0 0 πΌ † [ 0 0 πΊπΈ ] πΌ 0 ], 0 πΌ π2 = [ π4 = [ π4 = [ π» 0 ], πΌ 0 π3 = [ =[ (24) πΌ 0 ], 0 πΌ 0 πΌ π5 = [ † ] . πΈπΈ 0 πΌ π» ], 0 πΌ πΌ π» π1 π4 = [ ], 0 πΌ π2∗ π1 π4 = [ π» 0 π1 π2 π5 = [ ∗ (25) π ππ» (πΌ − πππ π † ) ], ∗ † −π π πππ» π π π − π π † πππ»∗ ππ» (πΌ − πππ π † ) =[ 0 ππ» (πΌ − πππ π † ) ππ† ], † † 0 π π ππ − π π † πππ»∗ ππ» (πΌ − πππ π † ) ππ† π2∗ π1 π4 † ∗ † † ∗ † = [(πΌ − π π 0ππ) π» π π π + (πΌ − π π ππ)0π» ππ» (πΌ − πππ π )] , π3 π5 = [ 0 π» ], 0 πΌ 0 πΌ+π» π» ]. 0 0 πΉπ΄† 0 0 πΌ 0 † † [ πΉ = 0 πΉπ 0 ] [−π»∗ πΌ] . † [ 0 0 πΉπΈ ] [ πΌ 0] † † † ∗ † = [0 π π ππ + (πΌ − π π ππ) π» ππ» (πΌ − πππ π )] . 0 Hence, πΉπ΄† 0 0 πΉ = [ 0 πΉπ † 0 ] † [ 0 0 πΉπ] † (27) π ππ» (πΌ − πππ π † ) ππ ] ∗ −πππ» π ππ − πππ»∗ ππ» (πΌ − πππ π † ) ππ] . † ∗ † πΌ − π π ππ [(πΌ − π π ππ) π» π ] [ ×[ πΌ −πΎ − πΎ1 𴆠0 ] ]+[ A† = πΊ† πΉ† = [ 0 πΌ 0 0 (28) (32) If π = 0, then πΎ1 = 0, π1 = πΌ, and π2 = πΌ such that π3 = πΌ + πΎππΈ ππ ππΈ πΎ∗ and π4 = π † π . Letting π = π3−1 , then one gets the expression of A# by using (13): π΄ π΅ ] πΆ π· π1 = [ πΌ −πΎ − πΎ1 π† 0 𴆠0 ] ][ ]+[ 0 πΌ 0 0 0 πΈ† 3 −π»∗ πΌ π΄ π΅ ×[ ]) [ ]. πΌ 0 πΆ π· 0 (31) Since π† 0 −π»∗ πΌ ×[ ][ ], πΌ 0 0 πΈ† 0 ππ† ], 0 0 π2∗ π1 π2 π5 ∗ Now, πΉ† possesses the following form according to (18): × ([ 0 ππ† ]. 0 0 π1 π2 π5 0 πΌ π3 π5 = [ † ] , (26) πΈπΈ 0 πΌ+π» π» ], 0 π2∗ π1 π2 π5 = [ A# = [ (30) † Simple computations show that ∗ πΌ 0 ], 0 πΌ π1 π4 † πΊπ΄ When π is full row rank, one gets ππ = 0 which implies π = 0, π1 = πΌ, π2 = πΌ, π3 = πΌ, and π4 = 0. Thus, π1 = [ πΌ π» ], 0 πΌ π3 = [ By short computations, one gets So, (19) is reduced to πΊ† = [ π −ππ»πππ π † ], −π π † πππ»∗ π π π † + π π † πππ»∗ ππ»πππ π † (29) π −ππΎππΈ π † π ], −π † π ππΈ πΎ∗ π π † π + π † π ππΈ πΎ∗ ππΎππΈ π † π π2 = [ 0 πΎ ], 0 0 πΌ 0 π4 = [ ∗ ] , πΎ πΌ π3 = [ π5 = [ πΌ 0 ], 0 πΌ 0 0 ], 0 πΈ† πΈ (33) Journal of Applied Mathematics 5 Μ = (πΌ + πΎππ πΎ∗ )−1 . where π which imply π4 π1 =[ (b) If πΈ = 0, π = 0, and π (π΅∗ ) ⊂ π (π∗ ), then π −ππΎππΈ π † π ], † ∗ † πΎ π − π π ππΈ πΎ π π π − (πΌ − π † π ππΈ ) πΎ∗ ππΎππΈ π † π ∗ π1 π2 π3 = [ π5 π3 π2∗ π1 = [ 0 ππΎ ], 0 −π † π ππΈ πΎ∗ ππΎ π΄ π΅ πΌ −πΎ 𴆠0 ] ] ([ ][ πΆ π· 0 πΌ 0 S† ×[ 0 0 ], πΈ† πΈπΎ∗ π −πΈ† πΈπΎ∗ ππΎππΈ π † π π4 π1 π2 π3 = [ π5 π3 π2∗ π1 π2 π3 A# = [ 0 ππΎ ], ∗ 0 πΎ ππΎ − π † π ππΈ πΎ∗ ππΎ 0 0 =[ ]. ∗ † 0 πΎ ππΎ − π π ππΈ πΎ∗ ππΎ Μ = (πΌ + π»ππ π»∗ )−1 . where π (c) If πΈ = 0, π = 0, and π (π΅) ⊂ π (π΄), π (πΆ) ⊂ π (π), π (π΅∗ ) ⊂ π (π∗ ), π (πΆ∗ ) ⊂ π (π΄∗ ), then 3 π΄(𴆠) π΄ + π΄π΄† πΎπ† π»∗ 𴆠π΄ −π΄π΄† πΎ(π† ) π] A =[ . 2 3 −π(π† ) π»∗ 𴆠π΄ π(π† ) π [ ] (40) (35) Proof. (a) Since πΈ = 0 and π = 0, by Theorem 3(b), one gets −ππΎ π −ππΎππΈ πΊ† = [ ] ππ ππΈ πΎ∗ π πΌ − ππ ππΈ πΎ∗ ππΎ πΌ # A† = [ Then, A† = πΊ† πΉ† = [ Μ Μ π −ππΎ Μ πΌ − ππ πΎ∗ ππΎ Μ ] ππ πΎ∗ π Μ Μ π π ππ»π 𴆠0 ]. ×[ †] [ ∗ Μ πΌ − π»∗ ππ»π Μ π 0 π −π» π (36) 3 Μ Μ π π ππ»π π΄ 0 ] [ ]) ×[ Μ πΌ − π»∗ ππ»π Μ π 0 π† −π»∗ π † π΄ π΅ ]. πΆ π· (37) Theorem 4. Let A be defined by (4), then the following statements are true. (41) Μ = πΌ, then the Since π (πΆ) ⊂ π (π), that is, ππ πΆ = 0, then π equality previously mentioned is simplified to A† = [ Μ Μ π΄ π΅ π −ππΎ ] ([ ∗Μ Μ ] πΆ π· ππ πΎ π πΌ − ππ πΎ∗ ππΎ ×[ Μ Μ π −ππΎ 𴆠0 ] ∗Μ ∗Μ ][ 0 π† ππ πΎ π πΌ − ππ πΎ ππΎ Μ Μ π π ππ»π × [ ∗Μ Μ π] . −π» π πΌ − π»∗ ππ»π Therefore, we have A# = [ 2 (34) So, (19) is reduced to † πΊπ΄ 0 0 [ ] × [ 0 πΊπ † 0 ] . † [ 0 0 πΊπΈ ] 3 Μ Μ π π ππ»π π΄ π΅ ]) [ ], ∗Μ ∗Μ πΆ π· −π» π πΌ − π» ππ»ππ (39) Μ Μ π −ππΎ πΌ 0 𴆠0 ] [ ∗ ] . (42) ∗Μ ∗Μ ][ 0 π† −π» πΌ ππ πΎ π πΌ − ππ πΎ ππΎ 3 By using A# = A(A† ) A, we have A# = [ π΄ π΅ ] πΆ π· 3 Μ Μ π −ππΎ πΌ 0 𴆠0 × ([ Μ πΌ − ππ πΎ∗ ππΎ Μ ] [ 0 π† ] [−π»∗ πΌ]) ππ πΎ∗ π π΄ π΅ ×[ ]. πΆ π· (43) (a) If πΈ = 0, π = 0, and π (πΆ) ⊂ π (π), then (b) Similarly to the proof of (a). (c) Since πΈ = 0 and π = 0, by Theorem 2(b), one gets π΄ π΅ ] A# = [ πΆ π· Μ Μ π −ππΎ 𴆠0 ] × ([ ∗Μ ∗Μ ][ 0 π† ππ πΎ π πΌ − ππ πΎ ππΎ 3 πΌ 0 π΄ π΅ × [ ∗ ]) [ ], −π» πΌ πΆ π· (38) A† = [ Μ Μ π −ππΎ 𴆠0 ] ∗Μ ∗Μ ][ 0 π† ππ πΎ π πΌ − ππ πΎ ππΎ Μ Μ π π ππ»π × [ ∗Μ Μ π] . −π» π πΌ − π»∗ ππ»π (44) 6 Journal of Applied Mathematics Since π (π΅) ⊂ π (π΄), π (πΆ) ⊂ π (π), π (π΅∗ ) ⊂ π (π∗ ), π (πΆ∗ ) ⊂ π (π΄∗ ), that is, ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, π΅ππ = 0, then the previous equality is simplified to (b) If π΄ and π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, Bππ = 0, then A# πΌ −πΎ 𴆠0 πΌ 0 A =[ ][ ∗ ] ][ 0 πΌ 0 π† −π» πΌ † =[ (45) 𴆠+ πΎπ† π»∗ −πΎπ† ]. =[ −π† π»∗ π† π΄# + π΄# π΅π# πΆπ΄# 2 ππ πΆπ΄# (πΌ + π΄# π΅π# πΆ) π΄# − π# πΆπ΄# (πΌ − ππ πΆ(π΄# ) π΅) π# (c) Let π΄ and π be group inverse; then ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, and π΅ππ = 0 if and only if π΄ π΅ 𴆠+ πΎπ† π»∗ −πΎπ† AA = [ ] ][ πΆ π· −π† π»∗ π† † π΄π΄† + π΄πΎπ† π»∗ − π΅π† π»∗ −π΄πΎπ† + π΅π† =[ † ] πΆπ΄ + πΆπΎπ† π»∗ − π·π† π»∗ −πΆπΎπ† + π·π† A† A = [ =[ A# = [ π΄π΄† 0 ], 0 ππ† † ∗ † π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# ]. −π# πΆπ΄# π# (50) Proof. (i) If ππ΄π΅ = 0 and πΆππ΄ = 0, then πΈ, π, π defined in (8) can be simplified to πΈ = 0, π = 0; π = π and then there is a full rank factorization 𴆠+ πΎπ† π»∗ −πΎπ† π΄ π΅ ][ ] πΆ π· −π† π»∗ π† † ] (49) Moreover, =[ −π΄# π΅π# † ∗ † π΄ π΄ + πΎπ π» π΄ − πΎπ πΆ πΎ + πΎπ π» π΅ − πΎπ π· ] −π† π»∗ π΄ + π† πΆ −π† π»∗ π΅ + π† π· A=[ 0 πΊπ΄ πΊπ΄ π΄# π΅ πΉ π΄ π΅ ][ ] ] = πΉπΊ = [ #π΄ πΆ π· πΆπ΄ πΉπ΄ πΉπ 0 Gπ (51) according to (11). Thus, 𴆠π΄ 0 ]. =[ 0 π† π πΊπΉ = [ (46) πΊπ΄πΉπ΄ + πΊπ΄ πΎπΆπ΄# πΉπ΄ πΊπ΄ πΎπΉπ ], πΊπ π»πΉπ΄ πΊπ πΉπ (52) Therefore, where π» = πΆπ΄# and πΎ = π΄# π΅. Denote by πσΈ the Schur complement of πΊπ πΉπ in the partitioned matrix πΊπΉ. Then, π΄π΄† 0 A = AA A A A = [ ] 0 ππ† # † ×[ † † 𴆠+ πΎπ† π»∗ −πΎπ† 𴆠π΄ 0 ][ ] 0 π† π −π† π»∗ π† 3 −1 πσΈ = πΊπ΄πΉπ΄ + πΊπ΄ πΎπ»πΉπ΄ − πΊπ΄ πΎπΉπ (πΊπ πΉπ ) πΊπ π»πΉπ΄ = πΊπ΄πΉπ΄ + πΊπ΄ πΎπ»πΉπ΄ − πΊπ΄ πΎππ# π»πΉπ΄ 2 π΄(𴆠) π΄ + π΄π΄† πΎπ† π»∗ 𴆠π΄ −π΄π΄† πΎ(π† ) π] = [ . 2 3 π(π† ) π −π(π† ) π»∗ 𴆠π΄ [ ] (47) Theorem 5. Let A be defined by (4); let π = π· − πΆπ΄# π΅ be the Schur complement of π· in A; then the following statements are true. (a) If π΄ and π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, and ππ πΆ = 0, then A# = πΊπ΄πΉπ΄ + πΊπ΄ πΎππ π»πΉπ΄ (53) = πΊπ΄πΉπ΄ + πΊπ΄ πΎππ πΆπ΄# πΉπ΄ = πΊπ΄πΉπ΄ . Applying the Banachiewicz-Schur formula, we have (πΊπ΄ πΉπ΄) −1 −1 # # # # # # # # # # π΄ + π΄ π΅π πΆπ΄ π΄ (πΌ + π΅π πΆπ΄ ) π΄ π΅ππ − π΄ π΅π =[ ]. 2 −π# πΆπ΄# π# (πΌ − πΆ(π΄# ) π΅ππ ) (48) −1 (πΊπ΄ πΉπ΄ ) =[ −(πΊπ΄ πΉπ΄ ) πΊπ΄ πΎπΉπ (πΊπ πΉπ ) −1 −1 −(πΊπ πΉπ ) πΊπ π»πΉπ΄ (πΊπ΄ πΉπ΄ ) =[ −1 (πΊπ΄ πΉπ΄ ) # # −1 −1 −1 −1 (πΊπ πΉπ ) (πΌ + πΊπ π»πΉπ΄ (πΊπ΄ πΉπ΄ ) πΊπ΄ πΎπΉπ (πΊπ πΉπ ) ) −πΊπ΄ π΄# πΎπ# πΉπ −πΊπ π π»π΄ πΉπ΄ (πΊπ πΉπ ) −1 + πΊπ π# π»πΎπ# πΉπ ] ]. (54) Journal of Applied Mathematics 7 Simple computations give Short computations show that πΉ(πΊπΉ)−1 πΉ(πΊπΉ)−1 = [ =[ πΉπ΄ 0 ] π»πΉπ΄ πΉπ ×[ =[ ×[ −1 −πΊπ΄ π΄# πΎπ# πΉπ (πΊπ΄ πΉπ΄) ] −1 −πΊπ π# π»π΄# πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ π΄# πΉπ΄ −πΎπ# πΉπ ], 0 π# πΉπ (55) −1 −1 ×[ πΊπ΄ πΊπ΄ πΎ ] 0 πΊπ πΊπ΄ πΊπ΄ πΎ ] 0 πΊπ 0 πΊ π΄# =[ π΄ # ]. −πΊπ π π» πΊπ π# πΊπ΄ π΄# πΎππ πΊπ΄ π΄# ]. # # −πΊπ π π» πΊπ π − πΊπ π# π»πΎππ (61) Therefore, A# = πΉ(πΊπΉ)−2 πΊ Then, A# = πΉ(πΊπΉ)−2 πΊ =[ −πΎπ# πΉπ π΄# πΉπ΄ ], # ππ π»π΄ πΉπ΄ −ππ π»πΎπ# πΉπ + π# πΉπ (πΊπ΄ πΉπ΄) −πΊπ΄ π΄# πΎπ# πΉπ =[ ] −1 # # −πΊπ S π»π΄ πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ (πΊπ΄ πΉπ΄) −πΊπ΄π΄# πΎπ# πΉπ ] −1 # # −πΊπ π π»π΄ πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ ×[ =[ = [ −1 −πΊπ΄π΄# πΎπ# πΉπ (πΊπ΄ πΉπ΄) ], −1 −πΊπ π# π»π΄# πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ (πΊπΉ)−1 πΊ (πΊπΉ)−1 πΊ =[ πΉπ΄ 0 ] π»πΉπ΄ πΉπ =[ πΊπ΄ π΄# πΎππ πΊ π΄# π΄# πΉπ΄ −πΎπ# πΉπ ][ π΄ # ] # # 0 π πΉπ −πΊπ π π» πΊπ π − πΊπ π# π»πΎππ π΄# + π΄# π΅π# πΆπ΄# π΄# + π΄# π΅π# πΆπ΄# π΄# (πΌ + π΅π# πΆπ΄# ) π΄# π΅ππ − π΄# π΅π# =[ ]. 2 −π# πΆπ΄# π# (πΌ − πΆ(A# ) π΅ππ ) (56) (b) Since ππ΄π΅ = 0 and πΆππ΄ = 0, similar as (a), there is a full rank factorization of A such that A = πΉπΊ = [ πΉπ΄ 0 πΊπ΄ πΊπ΄π΄# π΅ ][ ]. # πΆπ΄ πΉπ΄ πΉπ 0 πΊπ (c) (⇒:) Since ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, and π΅ππ = 0, according to the proof of (a) and (b), we have πΉ(πΊπΉ)−1 = [ (57) π΄# πΉπ΄ −πΎπ# πΉπ ], 0 π# πΉπ −πΊπ΄ π΄# πΎππ# (πΊπ΄ πΉπ΄) ] (πΊπΉ)−1 πΊ = [ −1 # # −πΊπ π π»π΄ πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ ×[ = [ (59) = πΊπ΄ πΉπ΄. −1 −πΊπ΄ π΄# πΎπ# πΉπ (πΊπ΄ πΉπ΄) ] −1 # # −πΊπ π π»π΄ πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ −1 (58) By using π΅ππ = 0, one gets the Schur complement of πΊπ πΉπ in πΊπΉ: πσΈ = πΊπ΄ πΉπ΄ + πΊπ΄ π΄# π΅ππ π»πΉπ΄ πΉπ΄ 0 ] π»πΉπ΄ πΉπ ×[ = [ πΊ πΉ + πΊπ΄ πΎπΆπ΄# πΉπ΄ πΊπ΄ πΎπΉπ πΊπΉ = [ π΄ π΄ ]. πΊπ π»πΉπ΄ πΊπ πΉπ −π΄# π΅π# = [π πΆπ΄# (πΌ + π΄# π΅π# πΆ) π΄# − π# πΆπ΄# (πΌ − π πΆ(π΄# )2 π΅) π# ] . π π (62) We also have πΊπ΄ πΊπ΄ πΎ ] 0 πΊπ 0 πΊπ΄ π΄# ]. # −πΊπ π π» πΊπ π# (63) Hence, Hence, (πΊπΉ)−1 = [ −πΎπ# πΉπ 0 πΊπ΄ π΄# π΄# πΉπ΄ ] # # # ][ ππ π»π΄ πΉπ΄ −ππ π»πΎπ πΉπ + π πΉπ −πΊπ π# π» πΊπ π# −1 # # −πΊπ΄ π΄ πΎπ πΉπ (πΊπ΄ πΉπ΄) ]. −1 # # −πΊπ π π»π΄ πΉπ΄ (πΊπ πΉπ ) + πΊπ π# π»πΎπ# πΉπ (60) A# = πΉ(πΊπΉ)−1 (πΊπΉ)−1 πΊ = [ (⇐:) By [9, Theorem 2]. π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# ]. −π# πΆπ΄# π# (64) 8 Journal of Applied Mathematics Analogous to Theorem 5, if define π = π΄ − π΅π·# πΆ the Schur complement of π΄ in A, one can obtain the following results. Theorem 6. Let A be defined by (4); let π = π΄ − π΅π·# πΆ be the Schur complement of π΄ in A; then the following statements are true. (a) If π· and π are group inverse, ππ·πΆ = 0, π΅ππ· = 0, ππ π΅ = 0, then A# = [ 2 π# (πΌ − π΅(π·# ) πΆππ ) # # # # # −π# π΅π·# # # −π· πΆπ + π· (πΌ + πΆπ π΅π· ) π· πΆππ π· + π·# πΆπ# π΅π·# ]. (65) (b) If π· and π are group inverse, ππ·πΆ = 0, π΅ππ· = 0, and πΆππ = 0, then A# = [ 2 (πΌ − ππ π΅(π·# ) πΆ) π# −π# π΅π·# + ππ π΅π·# (πΌ + π·# πΆπ# π΅) π·# # # # −π· πΆπ # # # π· + π· πΆπ π΅π· (c) If π΄, π, π·, π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, π΅ππ = 0, ππ·πΆ = 0, π΅ππ· = 0, and ππ π΅ = 0, then A# = [ π΄# + π΄# π΅π# πΆπ΄# # # # −π΄# π΅π# # # # ππ πΆπ΄ (πΌ + π΄ π΅π πΆ) π΄ − π πΆπ΄ 2 (πΌ − ππ πΆ(π΄# ) π΅) π# 2 =[ π# (πΌ − π΅(π·# ) πΆππ ) # # # # # −π# π΅π·# # # −π· πΆπ + π· (πΌ + πΆπ π΅π· ) π· πΆππ π· + π·# πΆπ# π΅π·# (d) If π΄, π, π·, π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, π΅ππ = 0, ππ·πΆ = 0, π΅ππ· = 0, and πΆππ = 0, then A# = [ π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# 2 ππ πΆπ΄# (πΌ + A# π΅π# πΆ) π΄# − π# πΆπ΄# (πΌ − ππ πΆ(π΄# ) π΅) π# ] 2 (πΌ − ππ π΅(π·# ) πΆ) π# −π# π΅π·# + ππ π΅π·# (πΌ + π·# πΆπ# π΅) π·# ]. (c) Let π· and π be group inverse; then ππ·πΆ = 0, π΅ππ· = 0, πΆππ = 0, and ππ π΅ = 0 if and only if −π# π΅π·# π# ]. −π·# πΆπ# π·# + π·# πΆπ# π΅π·# ]. (70) =[ −π·# πΆπ# π·# + π·# πΆπ# π΅π·# Theorem 8. Let A be defined by (4); let π = π·−πΆπ΄# π΅, π = π΄− π΅π·# πΆ be the Schur complement of π· and π΄ in A, respectively. Then (67) A# = [ π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# ] −π# πΆπ΄# π# (72) π# −π# π΅π·# =[ # # # ] −π· πΆπ π· + π·# πΆπ# π΅π·# Proof. The proof is similar to the proof of Theorem 5. Combining Theorems 5 and 6, we have the following results. ]. (71) (66) A# = [ ] if and only if one of the following conditions holds # Theorem 7. Let A be defined by (4); let π = π·−πΆπ΄ π΅, π = π΄− π΅π·# πΆ be the Schur complement of π· and π΄ in A, respectively. Then the following statements are true. (a) ππ΄π΅ = 0, ππ·πΆ = 0, ππ πΆ = 0, πΆππ΄ = 0, π΅ππ· = 0, π΅ππ = 0, (a) If π΄, π, π·, π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, ππ·πΆ = 0, π΅ππ· = 0, and ππ π΅ = 0, then (b) ππ΄π΅ = 0, ππ·πΆ = 0, ππ π΅ = 0, # A =[ π΄# + π΄# π΅π# πΆπ΄# π΄# (πΌ + π΅π# πΆπ΄# ) π΄# π΅ππ − π΄# π΅π# 2 −π# πΆπ΄# π# (πΌ − πΆ(π΄# ) π΅ππ ) 2 π# (πΌ − π΅(π·# ) πΆππ ) =[ −π# π΅π·# ]. (b) If π΄, π, π·, π are group inverse, ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, ππ·πΆ = 0, π΅ππ· = 0, and πΆππ = 0, then A# = [ # # # # # # # # π΄ + π΄ π΅π πΆπ΄ π΄ (πΌ + π΅π πΆπ΄ ) π΄ π΅ππ − π΄ π΅π −π# πΆπ΄# π# (πΌ − πΆ(π΄# ) π΅ππ ) 2 2 ] −π·# πΆπ# π·# + π·# πΆπ# π΅π·# Proof. (a) Using Theorem 6(c) and Theorem 7(c), we conclude that ππ΄π΅ = 0, πΆππ΄ = 0, ππ πΆ = 0, ππ·πΆ = 0, π΅ππ· = 0, πΆππ = 0, ]. (69) π΅ππ = 0, πππ΅ = 0, (75) if and only if A# = [ (πΌ − ππ π΅(π·# ) πΆ) π# −π# π΅π·# + ππ π΅π·# (πΌ + π·# πΆπ# π΅) π·# =[ πΆππ = 0. (74) (68) # πΆππ΄ = 0, ] −π·# πΆπ# + π·# (πΌ + πΆπ# π΅π·# ) π·# πΆππ π·# + π·# πΆπ# π΅π·# # π΅ππ· = 0, (73) π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# ] −π# πΆπ΄# π# π# −π# π΅π·# =[ # # # ]. −π· πΆπ π· + π·# πΆπ# π΅π·# (76) Journal of Applied Mathematics 9 Now, we only need to prove (73) is equivalent to (75). Denote πσΈ = π΄# + π΄# π΅π# πΆπ΄# . Then ππσΈ = (π΄ − π΅π·# πΆ) (π΄# + π΄# π΅π# πΆπ΄# ) = π΄π΄# + π΄π΄# π΅π# πΆπ΄# − π΅π·# πΆπ΄# − π΅π·# πΆπ΄# π΅π# πΆπ΄# = π΄π΄# + π΅π# πΆπ΄# − π΅π·# πΆπ΄# − π΅π·# (π· − π) π# πΆπ΄# = π΄π΄# , Now, the solution of system (79) can be obtained by the two small linear systems previously mentioned. In that case, the operation can be significantly simplified. We will also notice that the Moore-Penrose inverse of π΄ can be replaced by other generalized inverses, such as the group inverse, the Drazin inverse and generalized inverse of π΄ or even the ordinary inverse π΄−1 . In the following, we will give the group inverse solutions of the linear system. Theorem 9. Let πσΈ π = (π΄# + π΄# π΅π# πΆπ΄# ) (π΄ − π΅π·# πΆ) Aπ₯ = π¦ = π΄# π΄ − π΄# π΅π·# πΆ − π΄# π΅π# πΆπ΄# π΄ − π΄# π΅π# πΆπ΄# π΅π·# πΆ = π΄# π΄ − π΄# π΅π·# πΆ − π΄# π΅π# πΆ − π΄# π΅π# (π· − π) π·# πΆ be a linear system. Suppose A satisfies all the conditions of Theorem 5 (c), partitioning π₯ and π¦ as = π΄# π΄. π₯ π₯ = [ 1] , π₯2 (77) Moreover, we have π₯1 = π΄# (π¦1 − π΅π₯2 ) , πσΈ ππσΈ = π΄# π΄ (π΄# + π΄# π΅π# πΆπ΄# ) = π΄# + π΄# π΅π# πΆπ΄# = πσΈ . (78) Thus, πσΈ = π# . Hence, π# π = π΄# π΄ and ππ# = π΄π΄# . Now, we get ππ΄π΅ = ππ π΅ = 0 and πΆππ΄ = πΆππ = 0, which means (73) implying (75). Obviously, (75) implies (73). So, (73) is equivalent to (75). (b) The proof is similar to (a). 3. Applications to the Solution of a Linear System (79) be a linear system. Applying the block Gaussian elimination to the system, we have π¦1 π΄ π΅ π₯ ]. ] [ 1] = [ π¦2 − πΆπ΄† π¦1 0 π· − πΆπ΄† π΅ π₯2 (80) Hence, we get π΄π₯1 + π΅π₯2 = π¦1 ; ππ₯2 = π¦2 − πΆπ΄† π¦1 . ππ₯2 = π¦2 − πΆπ΄† π¦1 . (84) (85) where π = π· − πΆπ΄# π΅. Proof. Since π¦ ∈ π (A), we conclude that π₯ = A# π¦ is the solution of linear system (79). By Theorem 5 (c), we can get the following: =[ π΄# + π΄# π΅π# πΆπ΄# −π΄# π΅π# π¦1 ][ ] π¦2 −π# πΆπ΄# π# π΄# π¦1 + π΄# π΅π# πΆπ΄# π¦1 − π΄# π΅π# π¦2 ] π# (π¦2 − πΆπ΄# π¦1 ) (86) π₯ = [ 1] . π₯2 Now, it is easy to see that the solution π₯ = A# π¦ can be expressed as π₯1 = π΄# (π¦1 − π΅π₯2 ) , π₯2 = π# (π¦2 − πΆπ΄# π¦1 ) , (87) which are also the group inverse solutions of the two small linear systems of (82), respectively. (81) That is, π΄π₯1 = π¦1 − π΅π₯2 , π₯2 = π# (π¦2 − πΆπ΄# π¦1 ) , π₯ = A# π¦ = [ In this section, we will give an application of the previous results above to the solution of a linear system. Using generalized Schur complement, we can split a larger system into two small linear systems by the following steps. Let [ π¦ π¦ = [ 1] π¦2 which have appropriate sizes with A. 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