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Further characterizations of the weak group inverse of matrices and the weak group matrix

  • 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

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  • 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 ACm×n by R(A), N(A), A and r(A), respectively. The index of ACn×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 ACn×n, PA and PA represent the orthogonal projections onto R(A) and R(A) respectively, i.e. PA=AA and PA=AA.

    For the readers' convenience, we will first recall the definitions of some generalized inverses. For ACm×n, the Moore-Penrose inverse A of A is the unique matrix XCn×m satisfying the following four Penrose equations [4,18]:

    (1)AXA=A,(2)XAX=X,(3)(AX)=AX,(4)(XA)=XA.

    A matrix XCn×m satisfying (2) is called an outer inverse of A and is denoted by A(2). For ACm×n, a matrix XCn×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 ACn×nk, denoted by AD, is the unique matrix XCn×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 ACn×n, denoted by A is defined in [2] as the unique matrix XCn×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 ACn×nk, denoted by A is defined in [19] as the unique matrix XCn×n satisfying XAX=X and R(X)=R(X)=R(Ak) [11,19,21,30]. The BT-inverse of ACn×n, denoted by A, which is defined in [1] written by (APA) [1,13]. The DMP-inverse of ACn×nk, written by AD, is defined in [14] as the unique matrix XCn×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=AAAD [14,31]. The CMP-inverse of ACn×nk, written by AC, is defined in [15] as the unique matrix XCn×n satisfying XAX=X,AX=AADAA and XA=AAADA. Moreover, it was proved that AC,=AAADAA [15,24]. The (B,C)-inverse of ACm×n, denoted by A(B,C) [8], is the unique matrix XCn×m satisfying XAB=B,CAX=C, N(X)=N(C) and R(X)=R(B), where B, CCn×m [3,8].

    The weak group inverse of ACn×nk was defined for the first time by Wang and Chen [22]:

    Definition 1.1 [22] Let ACn×nk. The weak group inverse A of A is the unique matrix XCn×n satisfying

    The weak group matrix was defined for the first time by Wang and Liu [23]:

    Definition 1.2 [23] Let ACn×nk. We say a weak group matrix if ACWGn, in which

    CWGn={A|AA=AA,ACn×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|ACn×n,r(A2)=r(A)},CPn={A|ACn×n,A2=A},COPn={A|ACn×n,A2=A=A},CEPn={A|ACn×n,AA=AA}={A|ACn×n,R(A)=R(A)},CUn={A|ACn×n,AA=AA=In},CHn={A|ACn×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 ACn×nk can be represented in the form:

    A=A1+A2=U(TS0N)U,A1:=U(TS00)U,A2:=U(000N)U, (2.1)

    where TCp×p is nonsingular with p:=r(T)=r(Ak), N is nilpotent of index k, and UCn×n is unitary. The representation of A given in (2.1) satisfies Ind(A1)1, Ak2=0, and A1A2=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 ACn×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 ACn×nk be as in (2.1). Then

    (a)A=U(TΔTΔSN(InpNN)SΔN(InpNN)SΔSN)U; (2.3)
    (b)AD=U(T1(Tk+1)1˜T00)U; (2.4)
    (2.5)
    (d)A=U(TΔ1TΔ1SN(PNPN)SΔ1N(PNPN)SΔ1SN)U,whereΔ1=[TT+S(PNPN)S]1; (2.6)
    (e)AD,=U(T1(Tk+1)1˜TNN00)U; (2.7)
    (f)A,D=U(TΔTΔTk˜T(InpNN)SΔ(InpNN)SΔTk˜T)U; (2.8)
    (g)AC,=U(TΔTΔTk˜TNN(InpNN)SΔ(InpNN)SΔTk˜TNN)U, (2.9)
    where˜T=k1j=0TjSNk1jandΔ=[TT+S(InpNN)S]1. (2.10)

    The notation ˜T and Δ are often used as follows.

    Lemma 2.3 [10,21,22] Let ACn×nk be as in (2.1). Then

    (a)AA=U(Ip00NN)U; (2.11)
    (2.12)
    (2.13)

    Lemma 2.4 [25] Let ACm×n, XCn×l and YCl×m. Then the following conditions are equivalent:

    (a) limλ0X(λIl+YAX)1Y exists;

    (b) r(XYAXY)=r(XY);

    (c) A(2)R(XY),N(XY) exists,

    in which case,

    limλ0X(λIl+YAX)1Y=A(2)R(XY),N(XY).

    Lemma 2.5 [16] Let ACn×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 ACn×nk. Then the following statements hold:

    (a) AA=PR(Ak),N((Ak)A);

    (b) AA=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 ACn×nk and XCn×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=k1j=0TjSNk1j.

    Let X=U(X1X2X3X4)U, from R(X)=R(Ak) and AX2=X, we have

    X=U(T1X200)U,

    where X2Cp×(np),p=r(Ak).

    Hence, XAk+1=U(T1X200)UU(Tk+1T˜T00)U=U(Tk˜T00)U=Ak.

    (c)(a). By R(X)=R(Ak), we have X=AkL for some LCn×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 X1Cp×p and X2Cp×(np),p=r(Ak). And by (Ak)A2X=(Ak)A, we have X1=T1,X2=T2S.

    Hence, X=U(T1T2S00)U=A.

    In the following theorem, we show the other characterizations of weak group inverse by AAA=A.

    Theorem 3.2 Let ACn×nk and XCn×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 AA2XCHn.

    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, ACPn.

    From R(X)=R(Ak) we get Ak=PXAk. Hence

    Ak=PXAk=XXAk=XAXXAk=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 =PAkCHn, then AA2X=A(A)ACHn. From XAX=X and R(XA)=R(Ak), we obtain R(X)=R(Ak).

    (d)(a). Using the core-EP decomposition of ACn×nk (2.1), we partition X as follows:

    X=U(X1X2X3X4)U,

    where X1Cp×p, X2Cp×(np), X3C(np)×p, X4C(np)×(np) 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=T1. Again note that AA2XCHn, moreover

    AA2X=U(TS0N)(TS0N)2(T1X200)U=U(TTTT2X2STST2X2)U,

    we have ST=(TT2X2) and X2=T2S. Hence X=U(T1T2S00)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 AAk+1=Ak.

    Theorem 3.3 Let ACn×nk and XCn×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=k1j=0TjSNk1j, we can let X=U(X1X200)U, where X1Cp×p, X2Cp×(np) and p=r(Ak).

    By conditions XAk+1=Ak and A2X=PAkA, we get

    X=U(T1T2S00)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(lk). Also the condition AX2=X in items (b) of Theorem 3.3 can be replaced by X=AtXt+1(t1).

    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, XA.

    But we have the following result.

    Theorem 3.6 Let ACn×nk and XCn×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 ACn×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(AAk)={0}. For any ηN((Ak))R(AAk), we get (Ak)η=0, η=AAkξ for some ξCn. Since Ind(A)=k, then Akξ=Ak+1ξ0 for some ξ0Cn. Since 0=(Ak)η=(Ak+1)Ak+1ξ0, we get Ak+1ξ0=0, that is η=AAkξ=AAk+1ξ0=0. Hence, N((Ak))R(AAk)={0}.

    From (X1X2)A=0, we get R(X1X2)N(A)N((Ak)). From N(X1)N((Ak)A) and N(X2)N((Ak)A), we get R(X1X2)R(AAk), that is R(X1X2)N((Ak))R(AAk)={0}. Hence, X1=X2 and X1=X2.

    Bott-Duffin defined the B-D inverse of ACn×n by A(1)(L)=PL(APL+PL)1=PL(APL+IPL)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 ACn×nk. Then

    A=(A2)(1)(R(Ak))A=(PAkA2PAk)+A.

    Proof. By (2.1), we have Ak=U(Tk˜T00)U, where ˜T=k1j=0TjSNk1j. Then PAk=Ak(Ak)+=U(I000)U. Thus

    (A2)(1)(R(Ak))A=PAk(A2PAk+IPAk)1A=U(I000)(T200I)1(TS0N)U=U(T1T2S00)U=A.

    By direct calculation, we can get A=(PAkA2PAk)+A.

    Example 3.9 (see [16], Example 3.1) Let A=(554321444321333321222210111101000012).

    Since Ind(A)=2, by Theorem 2.1 of [16] the error-free weak group inverse of A is

    A=A2(A4)+A=[2053382053387051352895676645135212533823338233381050110410411351520521087310410423926026413413313100115012002332100117320025265262110425521710421311311336540042121001194004443200212612615780082294004138580082891001].

    On the other hand,

    A2=(6565605030105656524426844444135205292927231451414131185111125),
    (A2)+=(6003/21868421/5467323/1735329/2482376/4763802/316636003/21868421/5467323/1735329/2482376/4763802/31663117/2186841/10934169/1988069/3124017/4163167/16095508/899275/16641030/2589697/2565772/5301179/9165235/99467/994305/198835/284185/1988125/1988196/2125109/3579476/5231143/5662164/4051227/2137),
    PA2=A2(A2)+=(145/15415/773/283/449/30815/7727/775/145/2215/1543/285/14141/28011/4013/2803/445/2211/4097/44073/4409/30815/15413/28073/440502/17593/3085/15451/28049/4401247/3080),
    (A2PA2+IPA2)1=(1483/1250167/3211068/15651304/27751271/4938179/3989383/1053197/281393/1691554/3763185/2982107/4623601/1171174/1001687/72819/1144160/1787380/2339373/114416/1431/10401601/1649157/2653298/3339139/100150/100153/910107/1430823/1039775/2273387/800812/1001291/2519774/6421332/931389/955),
    (PA2A2PA2)+=(1525/135255/169424/537671/1247456/159195/2704888/5257134/259159/473193/2411317/8964190/20381621/1001367/2002407/910417/1430665/4891197/1001041/1043/26287/1040199/1040111/104023/1040673/400495/2002381/3640521/5720467/6026184/2879158/272141/200297/145621/2288773/16016163/1542).

    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(IQ)=(AP)1(IQ) by using P=IAA and Q=IAA. Now we generalize this equation by other ways.

    Theorem 3.10 Let ACn×nk, a0, P=IAA and Q=IAA. Then the matrices A+aP and A+aQ are invertible. In addition, the following identities hold:

    (a) A=(A+aP)1(IQ);

    (b) A=(IP)(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 α1Cp, αN(A+aP), then

    (TS0N)(α1α2)=a(0T1ST2SN0I)(α1α2)

    Thus, α2=0 and α1=0 as a0, N is nilpotent and T is nonsingular.

    By (A+aP)A=[A+a(IAA)]A=AA=IQ, we get A=(A+aP)1(IQ).

    (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=IAA and Q=IAA. Then

    (A+12P)1=(361/338315/338938/22791544/17132419/87883083/8788179/338497/3381031/701742/1147117/1013868/20874/134/13511/338287/33823/338241/3385/265/26203/6761003/676227/676105/6761/131/1319/16931/169236/169173/1691/261/2651/676101/676589/67673/676),
    (A13Q)1=(29/338985/3382763/13524897/676788/375514/169211/338803/3384896/4535485/1131015/8011255/7144/134/131766/10017045/20021025/1001787/5355/265/2681/10441/52101/1047/261/131/131289/4004905/10011147/551650/6971/261/26201/1489699/1733399/4611733/2002),

    By direct calculation, we have (A+12P)1(IQ)=A and (IP)(A13Q)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 ACn×nk is its (Ak,(Ak)A)-inverse.

    Theorem 3.13 Let ACn×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

    AAAk=AAk+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 ACn×nk. Then

    (a) A=limλ0Ak[λIn+(Ak)Ak+2]1(Ak)A;

    (b) A=limλ0Ak(Ak)A[λIn+Ak+1(Ak)A]1;

    (c) A=limλ0[λIn+Ak(Ak)A2]1Ak(Ak)A;

    (d) A=limλ0Ak(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)=limλ0Ak[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)=limλ0Ak(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)=limλ0[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)=limλ0Ak(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+1170248λ15416940))/(λ3+7321998λ2+2183534272λ+1182621440),m14=(10(13623λ2+3506196λ156574880))/(λ3+7321998λ2+2183534272λ+1182621440),m15=(80(1079λ2+406501λ7052430))/(λ3+7321998λ2+2183534272λ+1182621440),m16=(10(3641λ2+2997820λ+43736000))/(λ3+7321998λ2+2183534272λ+1182621440);
    m21=(4(39125λ2+10701612λ20118560))/(λ3+7321998λ2+2183534272λ+1182621440),m22=(4(39125λ2+10701612λ20118560))/(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+12133149λ1357520))/(λ3+7321998λ2+2183534272λ+1182621440);
    m31=(2(61511λ2+13065592λ181941760))/(λ3+7321998λ2+2183534272λ+1182621440),m32=(2(61511λ2+13065592λ181941760))/(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+119298056λ51097280))/(λ3+7321998λ2+2183534272λ+1182621440);
    m41=(32(2547λ2+817790λ7107100))/(λ3+7321998λ2+2183534272λ+1182621440),m42=(32(2547λ2+817790λ7107100))/(λ3+7321998λ2+2183534272λ+1182621440),m43=(2(37247λ2+12070490λ+119399280))/(λ3+7321998λ2+2183534272λ+1182621440),m44=(8(7677λ2+2633554λ+71071000))/(λ3+7321998λ2+2183534272λ+1182621440),m45=(2(19455λ210346054λ+96656560))/(λ3+7321998λ2+2183534272λ+1182621440),m46=(4(4101λ2+15613162λ+45485440))/(λ3+7321998λ2+2183534272λ+1182621440);
    m51=(2(19993λ2+13103688λ45485440))/(λ3+7321998λ2+2183534272λ+1182621440),m52=(2(19993λ2+13103688λ45485440))/(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(701λ25533026λ+11592880))/(λ3+7321998λ2+2183534272λ+1182621440),m64=(4(289λ22033752λ+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

    limλ0M=limλ0A2[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 ACn×nk be as in (2.1). Then the following statements hold:

    (a) A=0A is nilpotent;

    (b) A=AA3=A;

    (c) A=ATCUp and ACEPn;

    (d) A=PAACOPn.

    (e) A=PAACOPn.

    Proof. Using the core-EP decomposition of A and (2.13).

    (a).A=0r(Ak)=p=0A is nilpotent.(b).A=A(T1T2S00)=(TS0N)T2=Ip and N=0A3=A.(c).A=A(T1T2S00)=(T0SN)T1=T,S=0 and N=0TCUp and ACEPn.(d).A=PAA=AA(T1T2S00)=(Ip00NN)T=Ip,S=0 and N=0ACOPn.(e).A=PAA=AA(T1T2S00)=(TΔTTΔSTΔSNN(InpNN)SΔTNN+(InpNN)SΔS(InpNN))S=SNN,NN=0,T1=TΔT and T2S=TΔSN=0,S=0 and T=IpACOPn.

    where Δ=[TT+S(InpNN)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 ACn×nk. Then the following statements hold:

    (a) A=A#ACCMn;

    (b) A= ACEPn;

    (c) A=AACEPn.

    Proof. The proof is based on the core-EP decomposition of A.

    (a). From (2.2) and (2.13), we have

    A=A#(T1T2S00)=(T1T2S00) and N=0ACCMn.

    (b). From (2.2) and (2.13), we get that

    (c). From (2.3) and (2.13), we have

    A=AU(T1T2S00)U=U(TΔTΔSN(InpNN)SΔN(InpNN)SΔSN)UTΔ=T1,TΔSN=T2S,S=SNN and N=0N=0 and S=0ACEPn,

    where Δ=[TT+S(InpNN)S]1.

    Theorem 4.3 Let ACn×nk be as in (2.1). Then the following statements hold:

    (a) A= S=0;

    (b) A=ADSN=0;

    (c) A=AS=0 and N2=0;

    (d) A=AD,SN2=0 and S=SNN;

    (e) A=A,DS=SNN and SN=0;

    (f) A=AC,S=SNN,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=[T1(T1)+T2S(T2S)]1.

    (d). By (2.7) and (2.13), we get that

    A=AD,U(T1T2S00)U=U(T1(Tk+1)1˜TNN00)UT2S=(Tk+1)1˜TNNSN2=0 and S=SNN,

    where ˜T=k1j=0TjSNk1j.

    (e). By (2.8) and (2.13), we have

    A=A,DU(T1T2S00)U=U(TΔTΔTk˜T(InpNN)SΔ(InpNN)SΔTk˜T)UT1=TΔ,S=SNN and T2S=TΔTk˜TS=SNN and Tk1S=˜TS=SNN and SN=0,

    where Δ=[TT+S(InpNN)S]1 and ˜T=k1j=0TjSNk1j.

    (f). By (2.9) and (2.13), we get that

    A=AC,U(T1T2S00)U=U(TΔTΔ(Tk)1˜TNN(InpNN)SΔ(InpNN)SΔ(Tk)1˜TNN)US=SNN and Tk1S=˜TNNS=SNN,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=AA. 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 ACn×nk be as in (2.1). Then the following statements are equivalent:

    (a) ACWGn;

    (b) SN=0;

    (c) (A2)=(A)2;

    (d) A commutes with A2;

    (e) r(AAk,(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(AAk)=r((A)2Ak)=r(Ak), we get that r(AAk,(A)2Ak)=r(Ak) can be equivalently expressed as R(AAk)=R((A)2Ak), that is: N((Ak)A)=N((Ak)A2).

    Hence, AA=AA if and only if r(AAk,(A)2Ak)=r(Ak) by Lemma 2.6.

    Theorem 5.3 Let ACn×nk. Then the following conditions are equivalent:

    (a) ACWGn;

    (b) ()tA= ()t+1A2(t1);

    (c) ()tA commutes with ()tA2(t1).

    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 ACn×nk. Then the following conditions are equivalent:

    (a) ACWGn;

    (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=k1j=0TjSNk1j.

    (a)(f). By (2.4) and (2.13), we have

    AAD=AA(TS0N)(T1(Tk+1)1˜T00)=(TS0N)(T1T2S00)(ITk˜T00)=(IT1S00)Tk˜T=T1SSN=0ACWGn,

    where ˜T=k1j=0TjSNk1j.

    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.



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