This paper is devoted to consider some new characteristics and properties of the weak group inverse and the weak group matrix. First, we characterize the weak group inverse of a square matrix based on its range space and null space. Also several different characterizations of the weak group inverse are presented by projection and the Bott-Duffin inverse. Then by using the core-EP decomposition, we investigate the relationships between weak group inverse and other generalized inverses. And some new characterizations of weak group matrix are obtained.
Citation: Hui Yan, Hongxing Wang, Kezheng Zuo, Yang Chen. Further characterizations of the weak group inverse of matrices and the weak group matrix[J]. AIMS Mathematics, 2021, 6(9): 9322-9341. doi: 10.3934/math.2021542
[1] | Zhimei Fu, Kezheng Zuo, Yang Chen . Further characterizations of the weak core inverse of matrices and the weak core matrix. AIMS Mathematics, 2022, 7(3): 3630-3647. doi: 10.3934/math.2022200 |
[2] | Xiaofei Cao, Yuyue Huang, Xue Hua, Tingyu Zhao, Sanzhang Xu . Matrix inverses along the core parts of three matrix decompositions. AIMS Mathematics, 2023, 8(12): 30194-30208. doi: 10.3934/math.20231543 |
[3] | Jinyong Wu, Wenjie Shi, Sanzhang Xu . Revisiting the m-weak core inverse. AIMS Mathematics, 2024, 9(8): 21672-21685. doi: 10.3934/math.20241054 |
[4] | Wanlin Jiang, Kezheng Zuo . Further characterizations of the $ m $-weak group inverse of a complex matrix. AIMS Mathematics, 2022, 7(9): 17369-17392. doi: 10.3934/math.2022957 |
[5] | Yang Chen, Kezheng Zuo, Zhimei Fu . New characterizations of the generalized Moore-Penrose inverse of matrices. AIMS Mathematics, 2022, 7(3): 4359-4375. doi: 10.3934/math.2022242 |
[6] | Wanlin Jiang, Kezheng Zuo . Revisiting of the BT-inverse of matrices. AIMS Mathematics, 2021, 6(3): 2607-2622. doi: 10.3934/math.2021158 |
[7] | Yongge Tian . Miscellaneous reverse order laws and their equivalent facts for generalized inverses of a triple matrix product. AIMS Mathematics, 2021, 6(12): 13845-13886. doi: 10.3934/math.2021803 |
[8] | Jin Zhong, Yilin Zhang . Dual group inverses of dual matrices and their applications in solving systems of linear dual equations. AIMS Mathematics, 2022, 7(5): 7606-7624. doi: 10.3934/math.2022427 |
[9] | Suthep Suantai, Suparat Kesornprom, Nattawut Pholasa, Yeol Je Cho, Prasit Cholamjiak . A relaxed projection method using a new linesearch for the split feasibility problem. AIMS Mathematics, 2021, 6(3): 2690-2703. doi: 10.3934/math.2021163 |
[10] | Hongjie Jiang, Xiaoji Liu, Caijing Jiang . On the general strong fuzzy solutions of general fuzzy matrix equation involving the Core-EP inverse. AIMS Mathematics, 2022, 7(2): 3221-3238. doi: 10.3934/math.2022178 |
This paper is devoted to consider some new characteristics and properties of the weak group inverse and the weak group matrix. First, we characterize the weak group inverse of a square matrix based on its range space and null space. Also several different characterizations of the weak group inverse are presented by projection and the Bott-Duffin inverse. Then by using the core-EP decomposition, we investigate the relationships between weak group inverse and other generalized inverses. And some new characterizations of weak group matrix are obtained.
Throughout this paper, we denote the set of m×n complex matrices by Cm×n. And denote the identity matrix of order n by In, the range space, the null space, the conjugate transpose and the rank of the matrix A∈Cm×n by R(A), N(A), A∗ and r(A), respectively. The index of A∈Cn×n, denoted by Ind(A), is the smallest nonnegative integer k such that r(Ak)=r(Ak+1). The subset of Cn×n with index k will be denoted by Cn×nk. PL,M stands for the projector (idempotent) on the subspace L along the subspace M. For A∈Cn×n, PA and PA∗ represent the orthogonal projections onto R(A) and R(A∗) respectively, i.e. PA=AA† and PA∗=A†A.
For the readers' convenience, we will first recall the definitions of some generalized inverses. For A∈Cm×n, the Moore-Penrose inverse A† of A is the unique matrix X∈Cn×m satisfying the following four Penrose equations [4,18]:
(1)AXA=A,(2)XAX=X,(3)(AX)∗=AX,(4)(XA)∗=XA. |
A matrix X∈Cn×m satisfying (2) is called an outer inverse of A and is denoted by A(2). For A∈Cm×n, a matrix X∈Cn×m satisfying XAX=X, R(X)=T and N(X)=S, is denoted by A(2)T,S [6], where T is a subspace of Cn and S is a subspace of Cm. If A(2)T,S exists then it is unique.
The Drazin inverse of A∈Cn×nk, denoted by AD, is the unique matrix X∈Cn×n satisfying the following three equations [4,9]:
(5)AX2=X,(6)AX=XA,(7)XAk+1=Ak. |
In particular, if Ind(A)=1, then the Drazin inverse of A is called the group inverse of A and is denoted by A#. The core-inverse of A∈Cn×n, denoted by A is defined in [2] as the unique matrix X∈Cn×n satisfying AX=PA and R(X)⊆R(A). A
exists if and only if Ind(A)=1 [2,20]. The core-EP inverse of A∈Cn×nk, denoted by A
is defined in [19] as the unique matrix X∈Cn×n satisfying XAX=X and R(X)=R(X∗)=R(Ak) [11,19,21,30]. The BT-inverse of A∈Cn×n, denoted by A⋄, which is defined in [1] written by (APA)† [1,13]. The DMP-inverse of A∈Cn×nk, written by AD,† is defined in [14] as the unique matrix X∈Cn×n satisfying XAX=X,XA=ADA and AkX=AkA†. Moreover, it was proved that AD,†=ADAA†. Also, the dual DMP-inverse of A was introduced in [14], namely A†,D=A†AAD [14,31]. The CMP-inverse of A∈Cn×nk, written by AC,† is defined in [15] as the unique matrix X∈Cn×n satisfying XAX=X,AX=AADAA† and XA=A†AADA. Moreover, it was proved that AC,†=A†AADAA† [15,24]. The (B,C)-inverse of A∈Cm×n, denoted by A(B,C) [8], is the unique matrix X∈Cn×m satisfying XAB=B,CAX=C, N(X)=N(C) and R(X)=R(B), where B, C∈Cn×m [3,8].
The weak group inverse of A∈Cn×nk was defined for the first time by Wang and Chen [22]:
Definition 1.1 [22] Let A∈Cn×nk. The weak group inverse AⓌ of A is the unique matrix X∈Cn×n satisfying
![]() |
The weak group matrix was defined for the first time by Wang and Liu [23]:
Definition 1.2 [23] Let A∈Cn×nk. We say a weak group matrix if A∈CWGn, in which
CWGn={A|AAⓌ=AⓌA,A∈Cn×nk}. |
Recently, the study of the weak group inverse and the generalized weak group inverse has received a lot of attention (see e.g. [16,17,26,27,28]).
In this paper, we discuss some new characterizations and properties of the weak group inverse and the weak group matrix. First, we characterize the weak group inverse of a square matrix based on its range space and null space. Several different characterizations of the weak group inverse are presented by projection and the Bott-Duffin inverse. We also give the limit representations for the weak group inverse. Then we study the relationships between AⓌ and other generalized inverses such as A#, , A†,
, AD,AD,†. And some characterizations of the weak group matrix are obtained.
The research is arranged as follows. In Section 2, some indispensable matrix classes and lemmas are given. In Section 3, some characterizations of AⓌ are presented. In Section 4, we discuss the relationships between AⓌ and other generalized inverses by core-EP decomposition. Finally, we study the characterizations of the weak group matrix.
For convenience, some matrix classes will be given as follows.
These symbols CCMn,CPn,COPn,CEPn,CUn and CHn will stand for the subsets of Cn×n consisting of core matrices, projectors (idempotent matrices), orthogonal projectors (Hermitian idempotent matrices), EP-matrices (Range-Hermitian matrices), unitary matrices and Hermitian matrices, respectively, i.e.,
CCMn={A|A∈Cn×n,r(A2)=r(A)},CPn={A|A∈Cn×n,A2=A},COPn={A|A∈Cn×n,A2=A=A∗},CEPn={A|A∈Cn×n,AA†=A†A}={A|A∈Cn×n,R(A)=R(A∗)},CUn={A|A∈Cn×n,AA∗=A∗A=In},CHn={A|A∈Cn×n,A=A∗}. |
In order to study the characterizations and properties of the weak group inverse and the weak group matrix, we need to recall the core-EP decomposition of A, which plays an important role in this paper.
According to Theorem 2.2 in [21], every matrix A∈Cn×nk can be represented in the form:
A=A1+A2=U(TS0N)U∗,A1:=U(TS00)U∗,A2:=U(000N)U∗, | (2.1) |
where T∈Cp×p is nonsingular with p:=r(T)=r(Ak), N is nilpotent of index k, and U∈Cn×n is unitary. The representation of A given in (2.1) satisfies Ind(A1)≤1, Ak2=0, and A∗1A2=A2A1=0 [21, Theorem 2.1]. Moreover, it is unique [21, Theorem 2.4] and is called the core-EP decomposition of A.
Lemma 2.1 Let A∈Cn×nk be as in (2.1). Then
r(A)=r(A2)⟺N=0. |
In which case, we have
![]() |
(2.2) |
Proof. The proof is easy.
In [7,10,13,21,29], some generalized inverses such as A†,AD, , A⋄,AD,†,A†,D,AC,† can be represented by the core-EP decomposition of A. We list these results in the lemmas below.
Lemma 2.2 [7,10,13,21,29] Let A∈Cn×nk be as in (2.1). Then
(a)A†=U(T∗Δ−T∗ΔSN†(In−p−N†N)S∗ΔN†−(In−p−N†N)S∗ΔSN†)U∗; | (2.3) |
(b)AD=U(T−1(Tk+1)−1˜T00)U∗; | (2.4) |
![]() |
(2.5) |
(d)A⋄=U(T∗Δ1−T∗Δ1SN⋄(PN−PN⋄)S∗Δ1N⋄−(PN−PN⋄)S∗Δ1SN⋄)U∗,whereΔ1=[TT∗+S(PN−PN⋄)S∗]−1; | (2.6) |
(e)AD,†=U(T−1(Tk+1)−1˜TNN†00)U∗; | (2.7) |
(f)A†,D=U(T∗ΔT∗ΔT−k˜T(In−p−N†N)S∗Δ(In−p−N†N)S∗ΔT−k˜T)U∗; | (2.8) |
(g)AC,†=U(T∗ΔT∗ΔT−k˜TNN†(In−p−N†N)S∗Δ(In−p−N†N)S∗ΔT−k˜TNN†)U∗, | (2.9) |
where˜T=k−1∑j=0TjSNk−1−jandΔ=[TT∗+S(In−p−N†N)S∗]−1. | (2.10) |
The notation ˜T and Δ are often used as follows.
Lemma 2.3 [10,21,22] Let A∈Cn×nk be as in (2.1). Then
(a)AA†=U(Ip00NN†)U∗; | (2.11) |
![]() |
(2.12) |
![]() |
(2.13) |
Lemma 2.4 [25] Let A∈Cm×n, X∈Cn×l and Y∈Cl×m. Then the following conditions are equivalent:
(a) limλ→0X(λIl+YAX)−1Y exists;
(b) r(XYAXY)=r(XY);
(c) A(2)R(XY),N(XY) exists,
in which case,
limλ→0X(λIl+YAX)−1Y=A(2)R(XY),N(XY). |
Lemma 2.5 [16] Let A∈Cn×nk. Then
AⓌ=A(2)R(Ak),N((Ak)∗A)=A(2)R(Ak(Ak)∗A),N(Ak(Ak)∗A). |
Lemma 2.6 [17] Let A∈Cn×nk. Then the following statements hold:
(a) AAⓌ=PR(Ak),N((Ak)∗A);
(b) AⓌA=PR(Ak),N((Ak)∗A2).
Using the results of Lemma 2.5, we have R(AⓌ)=R(Ak) and N(AⓌ)=N((Ak)∗A). Now, we will give several different characterizations of the weak group inverse for a matrix A.
Theorem 3.1 Let A∈Cn×nk and X∈Cn×n. Then the following conditions are equivalent:
(a) X=AⓌ;
(b) R(X)=R(Ak),N(X)=N((Ak)∗A) and AX2=X;
(c) R(X)=R(Ak),N(X)=N((Ak)∗A) and XAk+1=Ak;
(d) R(X)=R(Ak) and AX= A;
(e) R(X)=R(Ak) and A2X=PAkA;
(f) R(X)=R(Ak) and (Ak)∗A2X=(Ak)∗A.
Proof. (a)⇒(b). The assertion follows directly from Lemma 2.5 and the definition of AⓌ.
(b)⇒(c). From (2.1), we can calculate that
Ak=U(Tk˜T00)U∗, |
where ˜T=k−1∑j=0TjSNk−1−j.
Let X=U(X1X2X3X4)U∗, from R(X)=R(Ak) and AX2=X, we have
X=U(T−1X200)U∗, |
where X2∈Cp×(n−p),p=r(Ak).
Hence, XAk+1=U(T−1X200)U∗⋅U(Tk+1T˜T00)U∗=U(Tk˜T00)U∗=Ak.
(c)⇒(a). By R(X)=R(Ak), we have X=AkL for some L∈Cn×n. Then we get that XAX=X since XAk+1=Ak. Hence, X=A(2)R(Ak),N((Ak)∗A)=AⓌ by Lemma 2.5.
(a)⇒(d). It can be obtained directly from Lemma 2.5 and the definition of AⓌ.
(d)⇒(e). Notice that A=PAk, which is obvious.
(e)⇒(f). From the condition, it follows that (Ak)∗A2X=(Ak)∗PAkA=(Ak)∗A.
(f)⇒(a). From (2.1) and R(X)=R(Ak), we can let X=U(X1X200)U∗, where X1∈Cp×p and X2∈Cp×(n−p),p=r(Ak). And by (Ak)∗A2X=(Ak)∗A, we have X1=T−1,X2=T−2S.
Hence, X=U(T−1T−2S00)U∗=AⓌ.
In the following theorem, we show the other characterizations of weak group inverse by AⓌAAⓌ=AⓌ.
Theorem 3.2 Let A∈Cn×nk and X∈Cn×n. Then the following conditions are equivalent:
(a) X=AⓌ;
(b) XAX=X,R(X)=R(Ak) and N(X)=N((Ak)∗A);
(c) XAX=X,R(XA)=R(Ak) and AX=A;
(d) XAX=X,R(X)=R(Ak) and A∗A2X∈CHn.
Proof. (a)⇒(b). We can obtain the assertion from Lemma 2.5.
(b)⇒(c). By XAX=X and R(X)=R(Ak), we can obtain that R(AX)=AR(X)=AR(Ak)=R(Ak+1)=R(Ak)=R(A) and N(AX)=N(X)=N((Ak)∗A)=N(
A). Hence AX =
A, since AX,
A∈CPn.
From R(X)=R(Ak) we get Ak=PXAk. Hence
Ak=PXAk=XX†Ak=XAXX†Ak=XAk+1. |
Thus, we have R(Ak)=R(XAk+1)⊆R(XA)⊆R(X)=R(Ak), we get R(XA)=R(Ak).
(c)⇒(d). Notice that A =PAk∈CHn, then A∗A2X=A∗(A
)A∈CHn. From XAX=X and R(XA)=R(Ak), we obtain R(X)=R(Ak).
(d)⇒(a). Using the core-EP decomposition of A∈Cn×nk (2.1), we partition X as follows:
X=U(X1X2X3X4)U∗, |
where X1∈Cp×p, X2∈Cp×(n−p), X3∈C(n−p)×p, X4∈C(n−p)×(n−p) and p=r(Ak).
By R(X)=R(Ak), we get that X=U(X1X200)U∗ and r(X1,X2)=p, the matrix (X1,X2) is full row rank. Thus, we have X1T=Ip by XAX=X. Hence X1=T−1. Again note that A∗A2X∈CHn, moreover
A∗A2X=U(TS0N)∗(TS0N)2(T−1X200)U∗=U(T∗TT∗T2X2S∗TS∗T2X2)U∗, |
we have S∗T=(T∗T2X2)∗ and X2=T−2S. Hence X=U(T−1T−2S00)U∗=AⓌ.
From Theorem 3.2, by R(AⓌ)=R(Ak) we know that AⓌ also satisfies the condition (7) in the definition of Drazin inverse. In the following theorem, we show some characterizations of AⓌ by AⓌAk+1=Ak.
Theorem 3.3 Let A∈Cn×nk and X∈Cn×n. Then the following conditions are equivalent:
(a) X=AⓌ;
(b) XAk+1=Ak,AX2=X and A2X=PAkA;
(c) XAk+1=Ak,AX= A and r(X)=r(Ak).
Proof. (a)⇒(b). By (2.13) and simple calculation, it is obvious.
(b)⇒(c). Since AX2=X, by induction it then follows that X=AX2=AXX=A(AX2)X=A2X3=⋯=AkXk+1. Thus, by Ak=U(Tk˜T00)U∗, where ˜T=∑k−1j=0TjSNk−1−j, we can let X=U(X1X200)U∗, where X1∈Cp×p, X2∈Cp×(n−p) and p=r(Ak).
By conditions XAk+1=Ak and A2X=PAkA, we get
X=U(T−1T−2S00)U∗ |
Thus AX= and r(X)=r(Ak).
(c)⇒(a). From XAk+1=Ak and r(X)=r(Ak), we have R(X)=R(Ak). XAX=X and R(XA)=R(Ak). Thus, by (c) of Theorem 3.2, we obtain that X=AⓌ.
Remark 3.4 Notice that the condition XAk+1=Ak in items (b) and (c) of Theorem 3.3 can be replaced by XAl+1=Al(l≥k). Also the condition AX2=X in items (b) of Theorem 3.3 can be replaced by X=AtXt+1(t≥1).
By Lemma 2.6, it is clear that AX=PR(Ak),N((Ak)∗A) and XA=PR(Ak),N((Ak)∗A2) when X=AⓌ. However, the conditions AX=PR(Ak),N((Ak)∗A) and XA=PR(Ak),N((Ak)∗A2) can not deduce that X=AⓌ. We will present the following example to illustrate that.
Example 3.5 Let
A=(100001000),X=(100002000), then AⓌ=(100000000). |
It is easy to check that k=Ind(A)=2, AX=PR(Ak),N((Ak)∗A) and XA=PR(Ak),N((Ak)∗A2). However, X≠AⓌ.
But we have the following result.
Theorem 3.6 Let A∈Cn×nk and X∈Cn×n. Then X=AⓌ if and only if X satisfies the following:
AX=PR(Ak),N((Ak)∗A),XA=PR(Ak),N((Ak)∗A2)andr(X)=r(Ak). |
Proof. If X=AⓌ, we can obtain the assertion directly by Lemma 2.6 and Theorem 3.3.
Conversely, by conditions R(XA)=R(Ak) and r(X)=r(Ak), we get R(X)=R(Ak) and XAX=X. Thus, N(X)=N(AX)=N((Ak)∗A). Therefore, X=AⓌ by Lemma 2.5.
The definition of AⓌ has been introduced from an algebraic approach. In [17], Dijana Mosic and Daochang Zhang characterized AⓌ by AX=PR(Ak),N((Ak)∗A),R(X)⊆R(Ak). In the following, we characterize AⓌ by the condition XA=PR(Ak),N((Ak)∗A2).
Theorem 3.7 Let A∈Cn×nk. Then AⓌ is the unique matrix X that satisfies:
XA=PR(Ak),N((Ak)∗A2),N(X)⊇N((Ak)∗A). | (3.1) |
Proof. AⓌ satisfies the two equations in (3.1) by Lemma 2.5 and Lemma 2.6. It remains to prove the uniqueness.
Suppose that X1,X2 satisfy (3.1). Then X1A=X2A, N(X1)⊇N((Ak)∗A) and N(X2)⊇N((Ak)∗A), we first show that N((Ak)∗)∩R(A∗Ak)={0}. For any η∈N((Ak)∗)∩R(A∗Ak), we get (Ak)∗η=0, η=A∗Akξ for some ξ∈Cn. Since Ind(A)=k, then Akξ=Ak+1ξ0 for some ξ0∈Cn. Since 0=(Ak)∗η=(Ak+1)∗Ak+1ξ0, we get Ak+1ξ0=0, that is η=A∗Akξ=A∗Ak+1ξ0=0. Hence, N((Ak)∗)∩R(A∗Ak)={0}.
From (X1−X2)A=0, we get R(X∗1−X∗2)⊆N(A∗)⊆N((Ak)∗). From N(X1)⊇N((Ak)∗A) and N(X2)⊇N((Ak)∗A), we get R(X∗1−X∗2)⊆R(A∗Ak), that is R(X∗1−X∗2)⊆N((Ak)∗)∩R(A∗Ak)={0}. Hence, X∗1=X∗2 and X1=X2.
Bott-Duffin defined the B-D inverse of A∈Cn×n by A(−1)(L)=PL(APL+PL⊥)−1=PL(APL+I−PL)−1 when APL+PL⊥ is nonsingular (see [5]). In [12], A is expressed by the B-D inverse. In the following, we use a special B-D inverse of A2 to express the weak group inverse of A.
Theorem 3.8 Let A∈Cn×nk. Then
AⓌ=(A2)(−1)(R(Ak))A=(PAkA2PAk)+A. |
Proof. By (2.1), we have Ak=U(Tk˜T00)U∗, where ˜T=∑k−1j=0TjSNk−1−j. Then PAk=Ak(Ak)+=U(I000)U∗. Thus
(A2)(−1)(R(Ak))A=PAk(A2PAk+I−PAk)−1A=U(I000)(T200I)−1⋅(TS0N)U∗=U(T−1T−2S00)U∗=AⓌ. |
By direct calculation, we can get AⓌ=(PAkA2PAk)+A.
Example 3.9 (see [16], Example 3.1) Let A=(55432144432133332122221011110−10000−1−2).
Since Ind(A)=2, by Theorem 2.1 of [16] the error-free weak group inverse of A is
AⓌ=A2(A4)+A=[205338205338−7051352−895676−6451352125338−23338−2333810501104104113515205210873104104−23926026−413−4133131001150120023321001−1732002−526−52621104255217104−213−113−11336540042121001−194004−4432002126126−1578008−2294004−13858008−2891001]. |
On the other hand,
A2=(6565605030105656524426844444135205292927231451414131185−1−1−1−125), |
(A2)+=(6003/21868−421/5467−323/1735−329/2482−376/4763−802/316636003/21868−421/5467−323/1735−329/2482−376/4763−802/31663−117/2186841/10934169/1988069/31240−17/4163−167/16095−508/899275/16641030/2589697/2565772/5301179/9165−235/99467/994305/198835/284185/1988125/1988196/2125−109/3579−476/5231−143/5662164/4051227/2137), |
PA2=A2(A2)+=(145/15415/77−3/28−3/44−9/30815/7727/775/145/2215/154−3/285/14141/28011/4013/280−3/445/2211/4097/44073/440−9/30815/15413/28073/440502/17593/308−5/154−51/28049/4401247/3080), |
(A2PA2+I−PA2)−1=(1483/1250−167/321−1068/1565−1304/2775−1271/4938−179/3989−383/1053197/281−393/1691−554/3763−185/2982107/4623−601/1171−174/1001687/72819/1144160/1787380/2339−373/1144−16/1431/10401601/1649−157/2653−298/3339−139/1001−50/100153/910−107/1430823/1039−775/2273387/800812/1001291/2519−774/6421−332/931389/955), |
(PA2A2PA2)+=(1525/1352−55/169−424/537−671/1247−456/1591−95/2704−888/5257−134/259159/473193/2411317/8964−190/20381−621/1001367/2002407/910417/1430665/4891−197/10010−41/1043/26287/1040199/1040111/104023/1040−673/400495/2002381/3640521/5720467/6026184/2879158/2721−41/2002−97/1456−21/2288773/16016163/1542). |
After simplification, it follows that A(2)(R(A2))A=AⓌ and (PA2A2PA2)+A=AⓌ.
In Theorem 2.2 of [16] the authors proved that AⓌ=(A+P)−1(I−Q)=(A−P)−1(I−Q) by using P=I−AⓌA and Q=I−AAⓌ. Now we generalize this equation by other ways.
Theorem 3.10 Let A∈Cn×nk, a≠0, P=I−AⓌA and Q=I−AAⓌ. Then the matrices A+aP and A+aQ are invertible. In addition, the following identities hold:
(a) AⓌ=(A+aP)−1(I−Q);
(b) AⓌ=(I−P)(A+aQ)−1.
Proof. (a) Firstly, we show that A+aP is invertible by (2.1) and (2.13).
Let α=U(α1α2)∈Cn, where α1∈Cp, α∈N(A+aP), then
(TS0N)(α1α2)=−a(0−T−1S−T−2SN0I)(α1α2) |
Thus, α2=0 and α1=0 as a≠0, N is nilpotent and T is nonsingular.
By (A+aP)AⓌ=[A+a(I−AⓌA)]AⓌ=AAⓌ=I−Q, we get AⓌ=(A+aP)−1(I−Q).
(b) It is similar to the proof of (a).
Remark 3.11 In the part (a) of Theorem 3.10, let a=±1, we have Theorem 2.2 of [16].
Example 3.12 Let A,AⓌ be the same as in example 3.9, P=I−AⓌA and Q=I−AAⓌ. Then
(A+12P)−1=(361/338−315/338938/2279−1544/1713−2419/87883083/8788−179/338497/338−1031/701742/1147117/1013−868/2087−4/13−4/13511/338−287/338−23/338241/338−5/26−5/26−203/6761003/676−227/676−105/676−1/13−1/13−19/169−31/169236/169−173/1691/261/2651/676101/676−589/67673/676), |
(A−13Q)−1=(−29/338985/3382763/1352−4897/676−788/375514/169211/338−803/338−4896/4535485/1131015/801−1255/714−4/13−4/13−1766/10017045/20021025/1001−787/535−5/26−5/2681/104−41/52101/104−7/26−1/13−1/131289/4004905/1001−1147/551650/6971/261/26−201/1489−699/1733399/461−1733/2002), |
By direct calculation, we have (A+12P)−1(I−Q)=AⓌ and (I−P)(A−13Q)−1=AⓌ.
In the following theorem we present a connection between (B,C)-inverse and weak group inverse, it shows that a weak group inverse of a matrix A∈Cn×nk is its (Ak,(Ak)∗A)-inverse.
Theorem 3.13 Let A∈Cn×nk. Then AⓌ=A(Ak,(Ak)∗A).
Proof. From the properties of weak group inverse (Lemma 2.5, Lemma 2.6 and Theorem 3.3), it follows that
AⓌA⋅Ak=AⓌAk+1=Ak,(Ak)∗AAAⓌ=(Ak)∗A,R(AⓌ)=R(Ak),N(AⓌ)=N((Ak)∗A). |
Hence AⓌ=A(Ak,(Ak)∗A).
In Theorem 3.1 of [16], the limit representation for the weak group inverse is derived using the limit representation of MP-inverse. In the following, the weak group inverse can also be characterized by Lemma 2.4.
Theorem 3.14 Let A∈Cn×nk. Then
(a) AⓌ=limλ→0Ak[λIn+(Ak)∗Ak+2]−1(Ak)∗A;
(b) AⓌ=limλ→0Ak(Ak)∗A[λIn+Ak+1(Ak)∗A]−1;
(c) AⓌ=limλ→0[λIn+Ak(Ak)∗A2]−1Ak(Ak)∗A;
(d) AⓌ=limλ→0Ak(Ak)∗[λIn+Ak+2(Ak)∗]−1A.
Proof. In the proof of the theorem, the results of Lemma 2.4 and Lemma 2.5 are used frequently.
(a). Let X=Ak,Y=(Ak)∗A. We have
AⓌ=A(2)R(Ak(Ak)∗A),N(Ak(Ak)∗A)=limλ→0Ak[λIn+(Ak)∗Ak+2]−1(Ak)∗A. |
(b). Let X=Ak(Ak)∗A,Y=In. Then
AⓌ=A(2)R(Ak(Ak)∗A),N(Ak(Ak)∗A)=limλ→0Ak(Ak)∗A[λIn+Ak+1(Ak)∗A]−1. |
(c). Let X=In,Y=Ak(Ak)∗A. Then
AⓌ=A(2)R(Ak(Ak)∗A),N(Ak(Ak)∗A)=limλ→0[λIn+Ak(Ak)∗A2]−1Ak(Ak)∗A. |
(d). Let X=Ak(Ak)∗, Y=A. Then
AⓌ=A(2)R(Ak(Ak)∗A),N(Ak(Ak)∗A)=limλ→0Ak(Ak)∗[λIn+Ak+2(Ak)∗]−1A. |
Example 3.15 Let A,AⓌ be the same as in example 3.9, M=A2[λI6+(A2)∗A4]−1(A2)∗A=(mij)6×6, where
m11=(10⋅(18079λ2+5552072λ+71727040))/(λ3+7321998λ2+2183534272λ+1182621440),m12=(10⋅(18079λ2+5552072λ+71727040))/(λ3+7321998λ2+2183534272λ+1182621440),m13=(40⋅(4131λ2+1170248λ−15416940))/(λ3+7321998λ2+2183534272λ+1182621440),m14=(10⋅(13623λ2+3506196λ−156574880))/(λ3+7321998λ2+2183534272λ+1182621440),m15=(80⋅(1079λ2+406501λ−7052430))/(λ3+7321998λ2+2183534272λ+1182621440),m16=(10⋅(3641λ2+2997820λ+43736000))/(λ3+7321998λ2+2183534272λ+1182621440); |
m21=(4⋅(39125λ2+10701612λ−20118560))/(λ3+7321998λ2+2183534272λ+1182621440),m22=(4⋅(39125λ2+10701612λ−20118560))/(λ3+7321998λ2+2183534272λ+1182621440),m23=(16⋅(8940λ2+2590793λ+7455710))/(λ3+7321998λ2+2183534272λ+1182621440),m24=(8⋅(14741λ2+4352547λ+32236840))/(λ3+7321998λ2+2183534272λ+1182621440),m25=(8⋅(9341λ2+8242848λ+15439660))/(λ3+7321998λ2+2183534272λ+1182621440),m26=(8⋅(3941λ2+12133149λ−1357520))/(λ3+7321998λ2+2183534272λ+1182621440); |
m31=(2⋅(61511λ2+13065592λ−181941760))/(λ3+7321998λ2+2183534272λ+1182621440),m32=(2⋅(61511λ2+13065592λ−181941760))/(λ3+7321998λ2+2183534272λ+1182621440),m33=(2⋅(56221λ2+15339222λ+184895360))/(λ3+7321998λ2+2183534272λ+1182621440),m34=(2⋅(46351λ2+13767572λ+443335360))/(λ3+7321998λ2+2183534272λ+1182621440),m35=(2⋅(29377λ2+66532814λ+196119040))/(λ3+7321998λ2+2183534272λ+1182621440),m36=(2⋅(12403λ2+119298056λ−51097280))/(λ3+7321998λ2+2183534272λ+1182621440); |
m41=(32⋅(2547λ2+817790λ−7107100))/(λ3+7321998λ2+2183534272λ+1182621440),m42=(32⋅(2547λ2+817790λ−7107100))/(λ3+7321998λ2+2183534272λ+1182621440),m43=(2⋅(37247λ2+12070490λ+119399280))/(λ3+7321998λ2+2183534272λ+1182621440),m44=(8⋅(7677λ2+2633554λ+71071000))/(λ3+7321998λ2+2183534272λ+1182621440),m45=(2⋅(19455λ2−10346054λ+96656560))/(λ3+7321998λ2+2183534272λ+1182621440),m46=−(4⋅(−4101λ2+15613162λ+45485440))/(λ3+7321998λ2+2183534272λ+1182621440); |
m51=(2⋅(19993λ2+13103688λ−45485440))/(λ3+7321998λ2+2183534272λ+1182621440),m52=(2⋅(19993λ2+13103688λ−45485440))/(λ3+7321998λ2+2183534272λ+1182621440),m53=(2⋅(18273λ2+8801758λ+53903200))/(λ3+7321998λ2+2183534272λ+1182621440),m54=(10⋅(3013λ2+1460172λ+25046528))/(λ3+7321998λ2+2183534272λ+1182621440),m55=−(2⋅(−9533λ2+87224922λ+2805920))/(λ3+7321998λ2+2183534272λ+1182621440),m56=−(2⋅(−4001λ2+181750704λ+130844480))/(λ3+7321998λ2+2183534272λ+1182621440); |
m61=(4⋅(−383λ2+6561368λ+11371360))/(λ3+7321998λ2+2183534272λ+1182621440),m62=(4⋅(−383λ2+6561368λ+11371360))/(λ3+7321998λ2+2183534272λ+1182621440),m63=−(2⋅(701λ2−5533026λ+11592880))/(λ3+7321998λ2+2183534272λ+1182621440),m64=−(4⋅(289λ2−2033752λ+16909360))/(λ3+7321998λ2+2183534272λ+1182621440),m65=−(2⋅(389λ2+164103790λ+102268400))/(λ3+7321998λ2+2183534272λ+1182621440),m66=−(8⋅(50λ2+83068771λ+42679520))/(λ3+7321998λ2+2183534272λ+1182621440); |
By direct calculation, we get
limλ→0M=limλ→0A2[λI6+(A2)∗A4]−1(A2)∗A=AⓌ. |
In this section, we first give some properties of weak group inverse by core-EP decomposition.
Theorem 4.1 Let A∈Cn×nk be as in (2.1). Then the following statements hold:
(a) AⓌ=0⟺A is nilpotent;
(b) AⓌ=A⟺A3=A;
(c) AⓌ=A∗⟺T∈CUp and A∈CEPn;
(d) AⓌ=PA⟺A∈COPn.
(e) AⓌ=PA∗⟺A∈COPn.
Proof. Using the core-EP decomposition of A and (2.13).
(a).AⓌ=0⟺r(Ak)=p=0⟺A is nilpotent.(b).AⓌ=A⟺(T−1T−2S00)=(TS0N)⟺T2=Ip and N=0⟺A3=A.(c).AⓌ=A∗⟺(T−1T−2S00)=(T∗0S∗N∗)⟺T−1=T∗,S=0 and N=0⟺T∈CUp and A∈CEPn.(d).AⓌ=PA⟺AⓌ=AA†⟺(T−1T−2S00)=(Ip00NN†)⟺T=Ip,S=0 and N=0⟺A∈COPn.(e).AⓌ=PA∗⟺AⓌ=A†A⟺(T−1T−2S00)=(T∗ΔTT∗ΔS−T∗ΔSN†N(In−p−N†N)S∗ΔTN†N+(In−p−N†N)S∗ΔS(In−p−N†N))⟺S=SN†N,N†N=0,T−1=T∗ΔT and T−2S=T∗ΔS⟺N=0,S=0 and T=Ip⟺A∈COPn. |
where Δ=[TT∗+S(In−p−N†N)S∗]−1.
It is well-known that A†=A# if and only if A is EP matrix. By the core-EP decomposition we will give the conditions which ensure that AⓌ=X, where X is one of A#, , A†,
, AD,A⋄,AD,†,AC,† and A†,D.
Theorem 4.2 Let A∈Cn×nk. Then the following statements hold:
(a) AⓌ=A#⟺A∈CCMn;
(b) AⓌ= ⟺A∈CEPn;
(c) AⓌ=A†⟺A∈CEPn.
Proof. The proof is based on the core-EP decomposition of A.
(a). From (2.2) and (2.13), we have
AⓌ=A#⟺(T−1T−2S00)=(T−1T−2S00) and N=0⟺A∈CCMn. |
(b). From (2.2) and (2.13), we get that
![]() |
(c). From (2.3) and (2.13), we have
AⓌ=A†⟺U(T−1T−2S00)U∗=U(T∗Δ−T∗ΔSN†(In−p−N†N)S∗ΔN†−(In−p−N†N)S∗ΔSN†)U∗⟺T∗Δ=T−1,−T∗ΔSN†=T−2S,S=SN†N and N†=0⟺N=0 and S=0⟺A∈CEPn, |
where Δ=[TT∗+S(In−p−N†N)S∗]−1.
Theorem 4.3 Let A∈Cn×nk be as in (2.1). Then the following statements hold:
(a) AⓌ= ⟺S=0;
(b) AⓌ=AD⟺SN=0;
(c) AⓌ=A⋄⟺S=0 and N2=0;
(d) AⓌ=AD,†⟺SN2=0 and S=SNN†;
(e) AⓌ=A†,D⟺S=SN†N and SN=0;
(f) AⓌ=AC,†⟺S=SN†N,SN2=0 and S=SNN†.
Proof. The core-EP decomposition of A is still our main tool.
(a). From (2.5) and (2.13), the result is obvious.
(b). See [10, Lemma 4.2, Theorem 4.3].
(c). By (2.3), (2.11) and (2.13), we have
![]() |
where Δ2=[T−1(T−1)∗+T−2S(T−2S)∗]−1.
(d). By (2.7) and (2.13), we get that
AⓌ=AD,†⟺U(T−1T−2S00)U∗=U(T−1(Tk+1)−1˜TNN†00)U∗⟺T−2S=(Tk+1)−1˜TNN†⟺SN2=0 and S=SNN†, |
where ˜T=k−1∑j=0TjSNk−1−j.
(e). By (2.8) and (2.13), we have
AⓌ=A†,D⟺U(T−1T−2S00)U∗=U(T∗ΔT∗ΔT−k˜T(In−p−N†N)S∗Δ(In−p−N†N)S∗ΔT−k˜T)U∗⟺T−1=T∗Δ,S=SN†N and T−2S=T∗ΔT−k˜T⟺S=SN†N and Tk−1S=˜T⟺S=SN†N and SN=0, |
where Δ=[TT∗+S(In−p−N†N)S∗]−1 and ˜T=k−1∑j=0TjSNk−1−j.
(f). By (2.9) and (2.13), we get that
AⓌ=AC,†⟺U(T−1T−2S00)U∗=U(T∗ΔT∗Δ(Tk)−1˜TNN†(In−p−N†N)S∗Δ(In−p−N†N)S∗Δ(Tk)−1˜TNN†)U∗⟺S=SN†N and Tk−1S=˜TNN†⟺S=SN†N,SN2=0 and S=SNN†, |
where Δ and ˜T are the same as in (e).
In [23], Wang and Liu introduced the weak group matrix defined by the commutability: AAⓌ=AⓌA. In this section we shall give different characterizations of weak group matrix by using the core-EP decomposition.
For convenience, we introduce a necessary lemma.
Lemma 5.1 [23] Let A∈Cn×nk be as in (2.1). Then the following statements are equivalent:
(a) A∈CWGn;
(b) SN=0;
(c) (A2)Ⓦ=(AⓌ)2;
(d) A commutes with
A2;
(e) r(A∗Ak,(A∗)2Ak)=r(Ak).
Remark 5.2 For (e) of Lemma 5.1, we give a short proof by using the properties of the weak group inverse.
Since r(A∗Ak)=r((A∗)2Ak)=r(Ak), we get that r(A∗Ak,(A∗)2Ak)=r(Ak) can be equivalently expressed as R(A∗Ak)=R((A∗)2Ak), that is: N((Ak)∗A)=N((Ak)∗A2).
Hence, AAⓌ=AⓌA if and only if r(A∗Ak,(A∗)2Ak)=r(Ak) by Lemma 2.6.
Theorem 5.3 Let A∈Cn×nk. Then the following conditions are equivalent:
(a) A∈CWGn;
(b) ()tA= (
)t+1A2(t≥1);
(c) ()tA commutes with (
)tA2(t≥1).
Proof. By the core-EP decomposition of A, we have
![]() |
Then, it is easy to prove these conclusions.
Remark 5.4 Let t=1 in (c) of Theorem 5.3, we get (d) of Lemma 5.1.
Theorem 5.5 Let A∈Cn×nk. Then the following conditions are equivalent:
(a) A∈CWGn;
(b) AkA†=Ak;
(c) Ak = AkAD,†;
(d) Ak=AkAⓌ;
(e) AAD= A;
(f) AAD=AAⓌ;
(g) A=AD,†A.
Proof. (a)⟺(c). By (2.5) and (2.7), we get that
![]() |
where ˜T=k−1∑j=0TjSNk−1−j.
(a)⟺(f). By (2.4) and (2.13), we have
AAD=AAⓌ⟺(TS0N)(T−1(Tk+1)−1˜T00)=(TS0N)(T−1T−2S00)⟺(IT−k˜T00)=(IT−1S00)⟺T−k˜T=T−1S⟺SN=0⟺A∈CWGn, |
where ˜T=k−1∑j=0TjSNk−1−j.
The rest of the proof is similar.
Our goal is to provide some new characterizations and properties of the weak group inverse and the weak group matrix by range space, null space, projection and the Bott-Duffin inverse. We also study the relationships between the weak group inverse and other generalized inverses such as A#, , A†,AD,AD,†.
We believe that research about the weak group inverse will be very popular in the next years. Some further investigations are proposed as follows:
1. Considering the weak group inverse of finite potent endomorphisms.
2. The applications of the weak group inverse in linear equations and matrix equations.
The authors are thankful to two anonymous referees for their careful reading, detailed corrections and pertinent suggestions on the first version of the paper, which enhanced the presentation of the results distinctly.
This research is supported by the Natural Science Foundation of China under Grants 11961076; the Science Foundation of Hubei Province Education Department (B2018148); the Youth Science Foundation of Hubei Normal University (HS2020QN031) and Thousands of Young and Middle-aged Key Teachers Training Programme in Guangxi Colleges and Universities.
All authors read and approved the final manuscript. The authors declare no conflict of interest.
[1] | O. M. Baksalary, G. Trenkler, On a generalized core inverse, Appl. Math. Comput., 236 (2014), 450–457. |
[2] |
O. M. Baksalary, G. Trenkler, Core inverse of matrices, Linear Multilinear Algebra, 58 (2010), 681–697. doi: 10.1080/03081080902778222
![]() |
[3] |
J. Benitez, E. Boasso, H. W. Jin, On one-side (B, C)-inverse of arbitrary matrices, Electron. J. Linear Algebra, 32 (2017), 391–422. doi: 10.13001/1081-3810.3487
![]() |
[4] | A. Ben-Israel, T. N. E. Greville, Generalized inverse: Theory and applications, 2 Eds., Springer Verlag, New-York, 2003. |
[5] |
R. Bott, R. J. Duffin, On the algebra of networks, Trans. Amer. Math. Soc., 74 (1953), 99–109. doi: 10.1090/S0002-9947-1953-0056573-X
![]() |
[6] | D. S. Cvetković-Ilić, Y. Wei, Algebraic properties of grneralized inverses, Series: Developments in Mathematics, Springer, 2017. |
[7] |
C. Y. Deng, H. K. Du, Representation of the Moore-Penrose inverse of 2×2 block operator valued matrices, J. Korean Math. Soc., 46 (2009), 1139–1150. doi: 10.4134/JKMS.2009.46.6.1139
![]() |
[8] |
M. P. Drazin, A class of outer generalized inverse, Linear Algebra Appl., 436 (2012), 1909–1923. doi: 10.1016/j.laa.2011.09.004
![]() |
[9] |
M. P. Drazin, Pseudo-inverse in associative rings and semigroups, Amer. Math. Mon., 65 (1958), 506–514. doi: 10.1080/00029890.1958.11991949
![]() |
[10] |
D. E. Ferreyra, F. E. Levis, N. Thome, Characterizations of k-commutative equalities for some outer generalized inverse, Linear Multiliear Algebra, 68 (2020), 177–192. doi: 10.1080/03081087.2018.1500994
![]() |
[11] |
D. E. Ferreyra, F. E. Levis, N. Thome, Revisiting the core-EP inverse and its extension to rectangular matrices, Quaest. Math., 41 (2018), 265–281. doi: 10.2989/16073606.2017.1377779
![]() |
[12] |
J. Ji, Y. M. Wei, The core-EP, weighted core-EP inverse of matrices and constrained systems of linear equations, Commun. Math. Res., 37 (2021), 86–112. doi: 10.4208/cmr.2020-0028
![]() |
[13] |
W. L. Jiang, K. Z. Zuo, Revisiting of the BT-inverse of matrices, AIMS Math., 6 (2021), 2607–2622. doi: 10.3934/math.2021158
![]() |
[14] | S. B. Malik, N. Thome, On a new generalized inverse for matrices of an arbitrary index, Appl. Math. Comput., 226 (2014), 575–580. |
[15] |
M. Mehdipour, A. Salemi, On a new generalized inverse of matrices, Linear Multilinear Algebra, 66 (2018), 1046–1053. doi: 10.1080/03081087.2017.1336200
![]() |
[16] | D. Mosić, P. S. Stanimirović, Representations for the weak group inverse, Appl. Math. Comput., 397 (2021), 125957. |
[17] |
D. Mosić, D. C. Zhang, Weighted weak group inverse for Hilbert space operators, Front. Math. China, 15 (2020), 709–726. doi: 10.1007/s11464-020-0847-8
![]() |
[18] |
R. A. Penrose, A generalized inverse for matrices, Math. Proc. Cambrige Philos. Soc., 51 (1955), 406–413. doi: 10.1017/S0305004100030401
![]() |
[19] |
K. M. Prasad, K. S. Mohana, Core-EP inverse, Linear Multilinear Algebra, 62 (2014), 792–802. doi: 10.1080/03081087.2013.791690
![]() |
[20] | D. S. Rakć, N. C. Dinˊciˊc, D. S. Djordjeviˊc, Core inverse and core partial order of Hilbert space operators, Appl. Math. Comput., 244 (2014), 283–302. |
[21] |
H. X. Wang, Core-EP decomposition and its applications, Linear Algebra Appl., 508 (2016), 289–300. doi: 10.1016/j.laa.2016.08.008
![]() |
[22] |
H. X. Wang, J. L. Chen, Weak group inverse, Open Math., 16 (2018), 1218–1232. doi: 10.1515/math-2018-0100
![]() |
[23] |
H. X. Wang, X. J. Liu, The weak group matrix, Aequationes math., 93 (2019), 1261–1273. doi: 10.1007/s00010-019-00639-8
![]() |
[24] | S. Z. Xu, J. L. Chen, D. Mosic, New characterzations of the CMP inverse of matrices, Linear Multilinear Algebra, 68 (2020), 796–804. |
[25] |
Y. X. Yuan, K. Z. Zuo, Compute limλ→0X(λIp+YAX)−1Y be the product singular value decomposition, Linear Multilinear Algebra, 64 (2016), 269–278. doi: 10.1080/03081087.2015.1034641
![]() |
[26] |
Y. K. Zhou, J. L. Chen, M. M. Zhou, m-weak group inverses in a ring with involution, RACSAM, 115 (2021), 1–13. doi: 10.1007/s13398-020-00944-x
![]() |
[27] | M. M. Zhou, J. L. Chen, Y. K. Zhou, Weak group inverses in proper ∗-rings, J. Algebra Appl., 19 (2021), 2050238. |
[28] | M. M. Zhou, J. L. Chen, Y. K. Zhou, N. Thome, Weak group inverses and partial isometris in proper ∗-rings, Linear Multilinear Algebra, (2021), 1884639. |
[29] |
K. Z. Zuo, O. M. Baksalary, D. S. Cvetkoviić-Ilić, Further characterizations of the co-EP matrices, Linear Algebra Appl., 616 (2021), 66–83. doi: 10.1016/j.laa.2020.12.029
![]() |
[30] |
K. Z. Zuo, Y. J. Cheng, The new revisitation of core-EP inverse of matrices, Filomat, 33 (2019), 3061–3072. doi: 10.2298/FIL1910061Z
![]() |
[31] | K. Z. Zuo, D. S. Cvetković-Ilić, Y. J. Cheng, Different characterizations of DMP-inverse of matrices, Linear Multilinear Algebra, 2020. DOI: 10.1080/03081087.2020.1729084. |
1. | Yang Chen, Kezheng Zuo, Zhimei Fu, New characterizations of the generalized Moore-Penrose inverse of matrices, 2022, 7, 2473-6988, 4359, 10.3934/math.2022242 | |
2. | Na Liu, Hongxing Wang, Efthymios G. Tsionas, The Characterizations of WG Matrix and Its Generalized Cayley–Hamilton Theorem, 2021, 2021, 2314-4785, 1, 10.1155/2021/4952943 | |
3. | Zhimei Fu, Kezheng Zuo, Yang Chen, Further characterizations of the weak core inverse of matrices and the weak core matrix, 2022, 7, 2473-6988, 3630, 10.3934/math.2022200 | |
4. | Dijana Mosić, Daochang Zhang, New Representations and Properties of the m-Weak Group Inverse, 2023, 78, 1422-6383, 10.1007/s00025-023-01878-7 | |
5. | Congcong Wang, Xiaoji Liu, Hongwei Jin, The MP weak group inverse and its application, 2022, 36, 0354-5180, 6085, 10.2298/FIL2218085W | |
6. | Dijana Mosić, Predrag S. Stanimirović, Lev A. Kazakovtsev, Application of m-weak group inverse in solving optimization problems, 2024, 118, 1578-7303, 10.1007/s13398-023-01512-9 | |
7. | Dijana Mosić, A generalization of the MP-m-WGI, 2024, 47, 1607-3606, 2133, 10.2989/16073606.2024.2352566 | |
8. | Dijana Mosić, Predrag S. Stanimirović, Lev A. Kazakovtsev, Minimization problem solvable by weighted m-weak group inverse, 2024, 1598-5865, 10.1007/s12190-024-02215-z | |
9. | Dijana Mosić, Daochang Zhang, Predrag S. Stanimirović, An extension of the MPD and MP weak group inverses, 2024, 465, 00963003, 128429, 10.1016/j.amc.2023.128429 | |
10. | Kezheng Zuo, Yang Chen, Li Yuan, Further representations and computations of the generalized Moore-Penrose inverse, 2023, 8, 2473-6988, 23442, 10.3934/math.20231191 | |
11. | D. Mosić, P. S. Stanimirović, L. A. Kazakovtsev, The $ m $-weak group inverse for rectangular matrices, 2024, 32, 2688-1594, 1822, 10.3934/era.2024083 | |
12. | Mengyu He, Xiaoji Liu, Hongwei Jin, The MPWG inverse of third-order F-square tensors based on the T-product, 2024, 38, 0354-5180, 939, 10.2298/FIL2403939H | |
13. | Jinzhao Wu, Hongjie Jiang, Mengyu He, Xiaoji Liu, General strong fuzzy solutions of complex fuzzy matrix equations involving the Moore-Penrose weak group inverse, 2024, 654, 00200255, 119832, 10.1016/j.ins.2023.119832 | |
14. | Shuangzhe Liu, Hongxing Wang, Yonghui Liu, Conan Liu, Matrix derivatives and Kronecker products for the core and generalized core inverses, 2024, 535, 0022247X, 128128, 10.1016/j.jmaa.2024.128128 | |
15. | Jiaxuan Yao, Hongwei Jin, Xiaoji Liu, The weak group-star matrix, 2023, 37, 0354-5180, 7919, 10.2298/FIL2323919Y | |
16. | Dijana Mosić, Janko Marovt, Weighted MP weak group inverse, 2024, 32, 1844-0835, 221, 10.2478/auom-2024-0012 | |
17. | Huanyin Chen, On m-Generalized Group Inverse in Banach $$*$$-Algebras, 2025, 22, 1660-5446, 10.1007/s00009-025-02818-1 |