Home Mathematics A note on the formulas for the Drazin inverse of the sum of two matrices
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A note on the formulas for the Drazin inverse of the sum of two matrices

  • Xin Liu EMAIL logo , Xiaoying Yang and Yaqiang Wang
Published/Copyright: March 26, 2019

Abstract

In this paper we derive the formula of (P + Q)D under the conditions Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0. Then, a corollary is given which satisfies the conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0. Meanwhile, we show that the additive formula provided by Bu et al. (J. Appl. Math. Comput. 38 (2012) 631-640) is not valid for all matrices which satisfies the conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0. Also, the representation can be simplified from Višnjić (Filomat 30 (2016) 125-130) which satisfies given conditions. Furthermore, we apply our result to establish a new representation for the Drazin inverse of a complex block matrix having generalized Schur complement equal to zero under some conditions. Finally, a numerical example is given to illustrate our result.

MSC 2010: 15A09

1 Introduction

Let Cn×n denote the set of all n × n complex matrices. For ACn×n, we call the smallest nonnegative integer k which satisfies rank(Ak+1) = rank(Ak) the index of A, and denote k by ind(A). Let ACn×n with ind(A) = k, we call the matrix XCn×n which satisfies

Ak+1X=Ak,XAX=X,XA=AX

the Drazin inverse of A and denote X by AD (see [1]). The Drazin inverse of a square complex matrix always exists and is unique (see [1]). In this paper, we denote Aπ = IAAD. A matrix ACn×n is nilpotent if Ak = 0 for some integer k ≥ 0. The smallest such k is called the index of nilpotency of A.

The Drazin inverse of square complex matrices has applications in several areas, such as singular differential or difference equations, Markov chains and iterative method and so on (see [1, 2]). For applications of the Drazin inverse of a 2 × 2 block matrix, we refer the readers to [2, 3, 4].

Suppose P, QCn×n. In 1958, Drazin offered the formula (P + Q)D = PD + QD, when PQ = QP = 0. In the recent years many authors have considered this problem and provided the representations of (P + Q)D with some specific conditions. In [5], the authors gave the representation of (P + Q)D when PQ = 0. In [6], the authors derived the formula for (P + Q)D under the conditions P2Q = 0, Q2 = 0. The case when P2Q = 0, Q2P = 0 was studied in [7]. In [8], the authors gave the formula for (P + Q)D when P2QP = 0, PQ2P = 0, P2Q2 = 0, PQ3 = 0. In [9], the formula of (P + Q)D under the conditions (P + Q)P(P + Q) = 0, QPQ2 = 0 was given. In [10], the authors derived a result under the conditions P(P + Q)Q = 0.

In this short paper, we derive the formula of (P + Q)D under the conditions Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0 in Section 3. We also get that a formula for (P + Q)D from [9] is not valid for all matrices which satisfy conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0. Meanwhile, a corollary is given which is valid for all matrices under the mentioned conditions. Furthermore, we offer an example which shows that the formula from [9] is not valid for all matrices which satisfy conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0.

Another aim of this paper is to derive a representation of the Drazin inverse of 2 × 2 complex block matrix

M=ABCD (1.1)

where A and D are square matrices. This problem was firstly posed in 1979 by Compbell and Meyer [11]. No formula for MD has yet been offered without any restrictions upon the blocks. Special cases of this problem have been studied. In some papers the expression of MD is given under conditions which concern the generalized Schur complement of matrix M defined by S = DCADB. Here we list some of them:

  1. CAπ = 0, AπB = 0, and S = 0 [12],

  2. CAπB = 0, AAπB = 0, and S = 0 [3],

  3. CAπB = 0, CAAπ = 0, and S = 0 [3],

  4. ABCAπ = 0, BCAπ is nilpotent, and S = 0 [6],

  5. AπBCA = 0, AπBC is nilpotent, and S = 0 [6],

  6. ABCAπ = 0, AπABC = 0, and S = 0 [7],

  7. ABCAπ = 0, CBCAπ = 0, and S = 0 [7],

  8. ABCAπA = 0, ABCAπB = 0, and S = 0 [8],

  9. AAπBCA = 0, CAπBCA = 0, and S = 0 [8].

    In Section 4, we derive a new representation for MD under the conditions ABCAπA = 0, AπBCA = 0, AπBCB = 0 and S = 0.

2 Some lemmas

In order to give the main results, we first give some lemmas as follows.

Lemma 2.1

[11] Let ACm×n, BCn×m, then

(AB)D=A(BA)D2B.

Lemma 2.2

[4] Let M=A0CB, where A and B are square matrices with ind(A) = r and ind(B) = s. Then max{r, s} ≤ ind(M) ≤ r + s, and

MD=AD0XBD,

where X=k=0s1BπBkC(AD)k+2+k=0r1(BD)k+2CAkAπBDCAD.

Lemma 2.3

[5] Let P, QCn×n be such that ind(P) = r and ind(Q) = s. If PQ = 0, then

(P+Q)D=i=0s1QπQi(PD)i+1+i=0r1(QD)i+1PiPπ.

Lemma 2.4

[13] Let P, QCn×n, such that ind(P) = r, ind(Q) = s. If PQP = 0 and PQ2 = 0, then

(P+Q)D=Y1+Y2+(Y1(PD)2+(QD)2Y2QD(PD)2(QD)2PD)PQ,

where Y1=i=0s1QπQi(PD)i+1,Y2=i=0r1(QD)i+1PiPπ.

Lemma 2.5

[6] Let P, QCn×n.

  1. If PQ = QP = 0, then (P + Q)D = PD + QD.

  2. If PQ = 0 and P is r-nilpotent, then ((P + Q)D)j = i=0r1 (QD)i+jPi, ∀j ≥ 1.

  3. If PQ = 0 and Q is s-nilpotent, then ((P + Q)D)j = i=0s1 Qi(PD)i+j, ∀j ≥ 1.

Lemma 2.6

[12] Let M be a matrix of the form (1.1), such that S = 0. If AπB = 0, CAπ = 0, then

MD=ICAD((AW)D)2AIADB,

where W = AAD + ADBCAD.

3 Additive results

In [9], Bu et al. gave the representation of (P + Q)D when (P + Q)P(P + Q) = 0, QPQ2 = 0 which is not correct for all matrices. In this paper we give the representation of (P + Q)D when Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0 are satisfied, from which we will get the correct formula under the conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0.

Theorem 3.1

Let P, QCn×n, if Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0, then

(P+Q)D=(P+Q)3((Q2+QP)D)2=(P+Q)2((Q2+QP)D)2(P+Q),

where

((Q2+QP)D)2=i=0t1QπQ2i((QP)D)i+2+i=0t1(QD)2(i+2)(QP)i(QP)π(QD)2(QP)D,

for t = max{ind(QP), ind(Q2)}.

Proof

Using definition of the Drazin inverse, we have that

(P+Q)D=(P+Q)((P+Q)2)D=(P+Q)IPQ+P2Q2+QPID. (3.1)

Denote by M=IPQ+P2Q2+QPI.

By Lemma 2.1 and Q(P + Q)P(P + Q) = 0, we have

MD=IPQ+P2Q2+QP0IPQ+P2D2Q2+QPI. (3.2)

Denote by

N=Q2+QP0IPQ+P2.

From P(P + Q)P(P + Q) = 0, we get (PQ + P2)D = 0. After applying Lemma 2.2 we get

ND=(Q2+QP)D0X0, (3.3)

where X = ((Q2 + QP)D)2 + (PQ + P2) ((Q2 + QP)D)3.

Since QPQ2 = 0 and Lemma 2.3, we obtain

(Q2+QP)D=i=0t1QπQ2i((QP)D)i+1+i=0t1(QD)2(i+1)(QP)i(QP)π,

where t = max{ind(QP), ind(Q2)}.

Substituting (3.3) into (3.2), we get

MD=(Q2+QP)D+(PQ+P2)(Q2+QP)D(Q2+QP).

By P(P + Q)P(P + Q) = 0, we have

MD=(Q2+QP)D+(PQ+P2)((Q2+QP)D)2. (3.4)

Substituting (3.4) into (3.1), we get

(P+Q)D=(P+Q)(Q2+QP)D+(P+Q)(PQ+P2)((Q2+QP)D)2=(P+Q)(Q2+QP)((Q2+QP)D)2+(P+Q)(PQ+P2)((Q2+QP)D)2=(P+Q)(P+Q)2((Q2+QP)D)2=(P+Q)3((Q2+QP)D)2.

Similarly, using definition of Drazin inverse, (P + Q)D = ((P + Q)2)D(P + Q).

So,

(P+Q)D=(P+Q)2((Q2+QP)D)2(P+Q).

The proof is completed.□

The next theorem is a symmetrical formulation of Theorem 3.1.

Theorem 3.2

Let P, QCn×n. If (P + Q)Q(P + Q)P = 0, (P + Q)P(P + Q)P = 0, Q2PQ = 0, then

(P+Q)D=(P+Q)3((Q2+PQ)D)2=(P+Q)2((Q2+PQ)D)2(P+Q),

where

((Q2+PQ)D)2=i=0t1(PQ)π(PQ)i((Q)D)2(i+2)+i=0t1((PQ)D)i+2Q2iQπ(PQ)D(QD)2,

for t = max{ind(PQ), ind(Q2)}.

Notice that one special case of Theorem 3.1 is when matrices P, Q satisfy the conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0, we get following additive formula.

Corollary 3.3

Let P, QCn×n, such that max{ind(QP), ind(Q2)} = t, if (P + Q)P(P + Q) = 0, QPQ2 = 0, then

(P+Q)D=(P+Q)2((Q2+QP)D)2(P+Q)=(P+Q)(Q2+QP)D,

where

(Q2+QP)D=i=0t1QπQ2i((QP)D)i+1+i=0t1(QD)2(i+1)(QP)i(QP)π,((Q2+QP)D)2=i=0t1QπQ2i((QP)D)i+2+i=0t1(QD)2(i+2)(QP)i(QP)π(QD)2(QP)D.

Remark 3.4

In [9, Theorem 3.1], the authors studied conditions from Corollary 3.3 and obtained the formula

(P+Q)D=(P+Q)2(i=0t1(QD)2i+4(QP)i(QP)π(QD)2(QP)D)(P+Q). (3.5)

Notice that in Corollary 3.3 we have additional element

(P+Q)2(i=0t1QπQ2i((QP)D)i+2)(P+Q).

In fact, this element doesn’t have to be equal to zero. So, the formula from [9] is not correct for all matrices which satisfy conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0.

Remark 3.5

In [10, Corollary 3.2], the author obtained the formula satisfy the same conditions from Corollary 3.3

(P+Q)D=(P+Q)2((Q2+QP)D)2(P+Q). (3.6)

Since (P + Q)P(P + Q) = 0, by Theorem 3.1, (3.6) can be checked easily that

(P+Q)D=(P+Q)3((Q2+QP)D)2=(P+Q)Q(P+Q)((Q2+QP)D)2+(P+Q)P(P+Q)((Q2+QP)D)2=(P+Q)(Q2+QP)D.

Next we consider matrices which satisfy conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0 and for which is (P+Q)2(i=0t1QπQ2i((QP)D)i+2)(P+Q)0. Furthermore, we demonstrate the application of Corollary 3.3.

Example 3.6

Let P and Q be matrices: P=0284,Q=0200.

It can be checked easily that (P + Q)P(P + Q) = 0, QPQ2 = 0. Hence the conditions of Corollary 3.3 are satisfied. Also, we have that (P+Q)2(i=0t1QπQ2i((QP)D)i+2)(P+Q)=0012140. Moreover, by the formula from Corollary 3.3, (P+Q)D=001214. But, if we apply the formula (3.5) from [9], we get that (P + Q)D = 0.

Example 3.7

[9] Let P and Q be matrices: P=0100000000010000,Q=0000111001011110.

It is obvious that (P + Q)P(P + Q) = 0, QPQ2 = 0. Hence the conditions of Corollary 3.3 are satisfied. After computation, we get

(QP)D=0,QD=0000121412141234121412141214,(Q2+QP)D=0000141414141414143414141414.

Moreover, by the formula from Corollary 3.3,

(P+Q)D=14141414121212123434343412121212.

But, in [9], the authors got that

(P+Q)D=1401401212121234034012121212.

This is illustrated easily by the definition of Drazin inverse, the result of (P + Q)D is not correct from [9].

4 A formula of the Drazin inverse for block matrix

In this section, we use the additive formula in section 3 to give representation for the Drazin inverse of a complex block matrix.

Let M=ABCD, where A and D are square matrices with generalized Schur complement S = DCADB of matrix M equal to zero. In [6], Martinez-Serrano and Castro-Gonzalez gave the representation for the Drazin inverse of M under the condition ABC = 0. In [7], Bu et al. gave the formula for MD under conditions ABCAπ = 0 and AπABC = 0. In the following Theorem 4.1, we give the representation for the Drazin inverse of M under the conditions ABCAπA = 0, AπBCA = 0, AπBCB = 0 and S = 0.

Theorem 4.1

Let M be a matrix of the form (1.1) such that S = 0. If ABCAπA = 0, AπBCA = 0 and AπBCB = 0, then

MD=LD+(LD)20AπB00+(LD)3AπBC000,

where

LD=AAADBCCADB(QD)2+AAADBCCADB(QD)4AADBCAπ0CADBCAπ0,(QD)n=ICAD((AW)D)n+1AIADB+((AAπ)D)n000,W=AAD+ADBCAD,forn1.

Proof

Consider the splitting of matrix M,

M=ABCCADB=AAADBCCADB+0AπB00.

If we denote by L=AAADBCCADB and H=0AπB00, we get H2 = 0, HD = 0. From AπBCA = 0, AπBCB = 0, it is obvious that HLH = 0, HL2 = 0. Hence, the conditions of Lemma 2.4 are satisfied, and

MD=(H+L)D=LD+(LD)2H+(LD)3HL. (4.1)

Let

Q=AAADBCAADCADB,P=00CAπ0,

then L = P + Q, P2 = 0. From ABCAπA = 0, we have Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0. Hence, the conditions of Theorem 3.1 are satisfied and

LD=(P+Q)D=(P+Q)(Q2+QP)D+(PQ+P2)((Q2+QP)D)2, (4.2)

where (Q2 + QP)D is defined as in Theorem 3.1.

Notice (QP)2 = 0, so (QP)D = 0. Thus ((Q2 + QP)D)n = (QD)2n + (QD)2n+2QP, n ≥ 1.

If we split matrix Q as

Q=A2ADAADBCAADCADB+AAπ000,

and denote by

Q1=A2ADAADBCAADCADB,Q2=AAπ000,

we get Q2Q1 = Q1Q2 = 0. After applying Lemma 2.5,

QD=(Q1)D+(Q2)D.

Let S1 be the generalized Schur complement of Q1, then we have

S1=CADBCAAD(A2AD)DAADB=0,

and

(A2AD)πAADB=0,CAAD(A2AD)π=0,

so from Lemma 2.6, we get

((Q1)D)n=ICAD((AW)D)n+1AIADB,

where W = AAD + ADBCAD, for n ≥ 1.

After computation we get

(QD)n=ICAD((AW)D)n+1AIADB+((AAπ)D)n000.

After substituting this expressions and (4.2) into (4.1), we complete the proof.□

5 Numerical example

The following numerical example illustrates the application of Theorem 4.1.

Example 5.1

Consider the matrix M=ABCD, where

A=1000000000000010,B=1000000000001000,C=0110100000000100,D=0000100000000000.

By computing we know the generalized Schur complement S = DCADB is zero and M satisfies the condition ABCAπA = 0, AπBCA = 0, AπBCB = 0, in Theorem 4.1 in the paper. We have ind(A) = 2, and

AD=1000000000000000,Aπ=0000010000100001,

then according to the formula in Theorem 4.1, we have

MD=1110100000000000000000000000000000000000111010000000000000000000.

6 Conclusions

In this paper we derive the formula of (P + Q)D under the conditions Q(P + Q)P(P + Q) = 0, P(P + Q)P(P + Q) = 0 and QPQ2 = 0. Then, a corollary is given which satisfies the conditions (P + Q)P(P + Q) = 0 and QPQ2 = 0. Furthermore, we apply the new result of (P + Q)D to establish a new representation for the Drazin inverse of complex block matrix having generalized Schur complement equal to zero under the conditions ABCAπA = 0, AπBCA = 0 and AπBCB = 0.

Acknowledgement

This work is supported by the Natural Science Foundation of Education Department of Sichuan Province(18ZB0521).

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Received: 2018-08-23
Accepted: 2019-01-03
Published Online: 2019-03-26

© 2019 Liu et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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  97. Algebraic and qualitative remarks about the family yy′ = (αxm+k–1 + βxmk–1)y + γx2m–2k–1
  98. On the two-term exponential sums and character sums of polynomials
  99. F-biharmonic maps into general Riemannian manifolds
  100. Embeddings of harmonic mixed norm spaces on smoothly bounded domains in ℝn
  101. Asymptotic behavior for non-autonomous stochastic plate equation on unbounded domains
  102. Power graphs and exchange property for resolving sets
  103. On nearly Hurewicz spaces
  104. Least eigenvalue of the connected graphs whose complements are cacti
  105. Determinants of two kinds of matrices whose elements involve sine functions
  106. A characterization of translational hulls of a strongly right type B semigroup
  107. Common fixed point results for two families of multivalued A–dominated contractive mappings on closed ball with applications
  108. Lp estimates for maximal functions along surfaces of revolution on product spaces
  109. Path-induced closure operators on graphs for defining digital Jordan surfaces
  110. Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras
  111. Existence of periodic solutions with prescribed minimal period of a 2nth-order discrete system
  112. Injective hulls of many-sorted ordered algebras
  113. Random uniform exponential attractor for stochastic non-autonomous reaction-diffusion equation with multiplicative noise in ℝ3
  114. Global properties of virus dynamics with B-cell impairment
  115. The monotonicity of ratios involving arc tangent function with applications
  116. A family of Cantorvals
  117. An asymptotic property of branching-type overloaded polling networks
  118. Almost periodic solutions of a commensalism system with Michaelis-Menten type harvesting on time scales
  119. Explicit order 3/2 Runge-Kutta method for numerical solutions of stochastic differential equations by using Itô-Taylor expansion
  120. L-fuzzy ideals and L-fuzzy subalgebras of Novikov algebras
  121. L-topological-convex spaces generated by L-convex bases
  122. An optimal fourth-order family of modified Cauchy methods for finding solutions of nonlinear equations and their dynamical behavior
  123. New error bounds for linear complementarity problems of Σ-SDD matrices and SB-matrices
  124. Hankel determinant of order three for familiar subsets of analytic functions related with sine function
  125. On some automorphic properties of Galois traces of class invariants from generalized Weber functions of level 5
  126. Results on existence for generalized nD Navier-Stokes equations
  127. Regular Banach space net and abstract-valued Orlicz space of range-varying type
  128. Some properties of pre-quasi operator ideal of type generalized Cesáro sequence space defined by weighted means
  129. On a new convergence in topological spaces
  130. On a fixed point theorem with application to functional equations
  131. Coupled system of a fractional order differential equations with weighted initial conditions
  132. Rough quotient in topological rough sets
  133. Split Hausdorff internal topologies on posets
  134. A preconditioned AOR iterative scheme for systems of linear equations with L-matrics
  135. New handy and accurate approximation for the Gaussian integrals with applications to science and engineering
  136. Special Issue on Graph Theory (GWGT 2019)
  137. The general position problem and strong resolving graphs
  138. Connected domination game played on Cartesian products
  139. On minimum algebraic connectivity of graphs whose complements are bicyclic
  140. A novel method to construct NSSD molecular graphs
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