The usual star, left-star, right-star, plus order, minus order and Lowner ordering have been
generalized to bimatrices. Also it is shown that all these orderings are partial orderings in bimatrices.
The relationship between star partial order and minus partial order of bimatrices and their squares are
examined.
1. International
OPEN ACCESS Journal
Of Modern Engineering Research (IJMER)
| IJMER | ISSN: 2249β6645 | www.ijmer.com | Vol. 4 | Iss.9| Sept. 2014 | 66|
On Some Partial Orderings for Bimatrices G. Ramesh1, N. Anbarasi2 1 Associate Professor of Mathematics, Govt Arts College (Auto), Kumbakonam 2Assistant Professor of Mathematics, Arasu Engineering College , Kumbakonam
I. Introduction And Preliminaries
Let βνν₯ν be the set of νν₯ν complex bimatrices. The symbols ν΄ν΅ β,β ν΄ν΅ and ν ν΄ν΅ denote the conjugate transpose, range space and rank subtractivity of ν΄ν΅ ν βνν₯ν respectively. Further, ν΄ν΅ β ν βνν₯ν stand for the Moore-Penrose inverse of ν΄ν΅[10], that is the unique bimatrix satisfying the equations, ν΄ν΅ ν΄ν΅ β ν΄ν΅=ν΄ν΅, ν΄ν΅ β ν΄ν΅ ν΄ν΅ β =ν΄ν΅ β ,ν΄ν΅ ν΄ν΅ β = ν΄ν΅ ν΄ν΅ β β , ν΄ν΅ β ν΄ν΅ = ν΄ν΅ β ν΄ν΅ β (1.1) and νΌν΅ν be the identity bimatrix of order ν. Moreover, βν νΈν , βν ν» and βν β₯denote the subsets of βνν₯ν consisting of νΈν, Hermitian, and Hermitian non-negative definite bimatrices respectively. That is, βν νΈν= ν΄ν΅ν βνν₯ν βΆν ν΄ν΅ =ν ν΄ν΅ β βΉν ν΄1 =ν ν΄1β ννν ν ν΄2 =ν ν΄2β βν ν»= ν΄ν΅ν βνν₯ν βΆν΄ν΅=ν΄ν΅ ββΉν΄1=ν΄1β ννν ν΄2=ν΄2β and βν β₯= ν΄ν΅ν βνν₯νβΆν΄ν΅=νΏν΅ νΏν΅ ββΉν΄1=νΏ1νΏ1β ; ν΄2=νΏ2νΏ2 β ννν ν ννννΏν΅=νΏ1βͺνΏ2ββνν₯ν In this paper, the usual star, left-star, right-star, plus order, minus order and Lowner order have been generalized to bimatrices. Also it is shown that all these orderings are partial orderings in bimatrices. The relationship between star partial order and minus partial order of bimatrices and their squares are examined. Definition 1.1 The star ordering for bimatrices is defined by,
ν΄ν΅β€βν΅ν΅βΊ ν΄ν΅ βν΄ν΅=ν΄ν΅ βν΅ν΅ that is, ν΄1βν΄1=ν΄1β ν΅1 ; ν΄2βν΄2=ν΄2βν΅2 and ν΄ν΅ν΄ν΅ β=ν΅ν΅ν΄ν΅ β that is, ν΄1ν΄1β =ν΅1ν΄1β ; ν΄2ν΄2β=ν΅2ν΄2β
and can alternatively be specified as, ν΄ν΅β€βν΅ν΅βΊ ν΄ν΅ β ν΄ν΅=ν΄ν΅ β ν΅ν΅ that is, ν΄1β ν΄1=ν΄1β ν΅1 ; ν΄2β ν΄2=ν΄2β ν΅2 and ν΄ν΅ν΄ν΅ β =ν΅ν΅ν΄ν΅ β that is, ν΄1ν΄1β =ν΅1ν΄1β ; ν΄2ν΄2β =ν΅2ν΄2β Example 1.2 Consider the bimatrices ν΄ν΅= 1 10 0 βͺ 2 20 0
(1.2)
(1.3)
Abstract: The usual star, left-star, right-star, plus order, minus order and Lowner ordering have been generalized to bimatrices. Also it is shown that all these orderings are partial orderings in bimatrices. The relationship between star partial order and minus partial order of bimatrices and their squares are examined.
Keywords: Star partial order, left-star partial order, right-star partial order, plus order, minus order and lowner order.
AMS Classification: 15A09, 15A15, 15A57
2. On Some Partial Orderings for Bimatrices
| IJMER | ISSN: 2249β6645 | www.ijmer.com | Vol. 4 | Iss.9| Sept. 2014 | 67|
and ν΅ν΅= 1 11 β1 βͺ 2 22 β2 βΉν΄ν΅β€βν΅ν΅ Definition 1.3 The left - star ordering for bimatrices is defined by,
ν΄ν΅ββ€ν΅ν΅βΊν΄ν΅ βν΄ν΅=ν΄ν΅ βν΅ν΅ that is, ν΄1β ν΄1=ν΄1β ν΅1 ; ν΄2βν΄2=ν΄2βν΅2 and β ν΄ν΅ ββ ν΅ν΅ that is, β ν΄1 ββ ν΅1 ; β ν΄2 ββ ν΅2 Definition 1.4
The right - star ordering for bimatrices is defined by,
ν΄ν΅β€βν΅ν΅βΊν΄ν΅ν΄ν΅ β=ν΅ν΅ν΄ν΅ β that is, ν΄1ν΄1β =ν΅1ν΄1β ; ν΄2ν΄2β=ν΅2ν΄2β and β ν΄ν΅ β ββ ν΅ν΅β that is, β ν΄1β ββ ν΅1β ; β ν΄2β ββ ν΅2β Definition 1.5 The plus - order for bimatrices is defined as, ν΄ν΅βν΅ν΅ whenever ν΄ν΅ β ν΄ν΅=ν΄ν΅ β ν΅ν΅ and ν΄ν΅ν΄ν΅ β =ν΅ν΅ν΄ν΅ β , for some reflexive generalized inverse ν΄ν΅ β of ν΄ν΅. ( satisfying both ν΄ν΅ν΄ν΅ β ν΄ν΅=ν΄ν΅ and ν΄ν΅ β ν΄ν΅ν΄ν΅ β =ν΄ν΅ β ). Definition 1.6 The minus (rank Subtractivity) ordering is defined for bimatrices as, ν΄ν΅β€β ν΅ν΅βΊ r(ν΅ν΅βν΄ν΅)=r ν΅ν΅ βr ν΄ν΅ that is, r(ν΅1βν΄1)= r ν΅1 β r ν΄1 and r(ν΅2βν΄2)= r ν΅2 β r ν΄2 (1.6) or as, ν΄ν΅β€β ν΅ν΅βΊ ν΄ν΅ν΅ν΅ β ν΅ν΅=ν΄ν΅, ν΅ν΅ν΅ν΅ β ν΄ν΅= ν΄ν΅ and ν΄ν΅ν΅ν΅ β ν΄ν΅=ν΄ν΅ (1.7) Note 1.7 i) It can be shown that, ν΄ν΅βν΅ν΅βΊ r(ν΅ν΅βν΄ν΅)=r ν΅ν΅ β r ν΄ν΅ and so the plus order is equivalent to rank subtractivity. ii) From (1.4) and (1.5) it is seen that ν΄ν΅β€βν΅ν΅βΊ ν΄ν΅ βββ€ ν΅ν΅β Definition 1.8 The Lowner partial ordering denoted by β€νΏ, for Which ν΄ν΅,ν΅ν΅ ν βννν is defined by ν΄ν΅β€νΏν΅ν΅βΊν΅ν΅βν΄ν΅ ν βν β₯. Result 1.9 Show that,the relation ββ€ is a partial ordering. Proof (1) ν΄ν΅ββ€ν΄ν΅βν΄1ββ€ν΄1 and ν΄2ββ€ν΄2 holds trivially. (2) If ν΄ν΅ βν΄ν΅= ν΄ν΅ βν΅ν΅ and β ν΅ν΅ β β ν΄ν΅ then ν΄ν΅=ν΄1βͺν΄2 = ν΄1β β ν΄1β ν΄1βͺ ν΄2β β ν΄2βν΄2 = ν΄1β β ν΄1β ν΅1βͺ ν΄2β β ν΄2βν΅2 = ν΄1 ν΄1β β ν΅1βͺ ν΄2 ν΄2β β ν΅2 =ν΅1βͺν΅2
(1.4)
(1.5)
3. On Some Partial Orderings for Bimatrices
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=ν΄ν΅=ν΅ν΅ (3) If ν΄ν΅ βν΄ν΅=ν΄ν΅ βν΅ν΅ and ν΅ν΅β ν΅ν΅=ν΅ν΅β νΆν΅ hold along with β ν΄ν΅ ββ ν΅ν΅ and β ν΅ν΅ ββ νΆν΅ ,then ν΄ν΅ βν΄ν΅=ν΄ν΅ βν΅ν΅ =ν΄1 βν΅1βͺν΄2 βν΅2 =ν΄1 βν΅1β β ν΅1β ν΅1βͺν΄2 βν΅2β β ν΅2β ν΅2 =ν΄1 βν΅1β β ν΅1β νΆ1βͺν΄2 βν΅2β β ν΅2β νΆ2 = ν΅1 ν΅1β ν΄1 β νΆ1βͺ ν΅2 ν΅2β ν΄2 β νΆ2 =ν΄1 βνΆ1βͺν΄2 βνΆ2 ν΄ν΅ β ν΄ν΅ =ν΄ν΅ β νΆν΅ ννν β ν΄ν΅ β β νΆν΅ Similarly, it can be verified that all the orderings are partial orderings. Lemma 1.10 [1] Let ν΄,ν΅ββνν₯ν and let ν=ν ν΄ <ν ν΅ =ν. Then ν΄β€βν΅ if and only if there exist νββνν₯ν,νβ βνν₯ν satisfying νβν=νΌν=ν βν, for which ν΄=ν ν·1 0 0 0 ν β and ν΅=ν ν·1 0 0 ν·2 ν β (1.8) where ν·1 and ν·2 are positive definite diagonal matrices of degree a and νβν, respectively. For ν΄,ν΅ββν ν», the matrix ν in (1.8) may be replaced by ν, but then ν·1 and ν·2 represent any nonsingular real diagonal matrices. Lemma 1.11[1] Let ν΄,ν΅ββνν₯ν and let ν=ν ν΄ <ν ν΅ =ν. Then ν΄β€βν΅ if only if there exist U ββνν₯ν, νββνν₯ν, satisfying ν βν=νΌν=ν βν, for which ν΄=ν ν·1 0 0 0 ν anda ν΅=ν ν·1+ν ν·2ν ν ν·2 ν·2ν ν·2 νβ (1.9) Where ν·1 and ν·2 are positive definite diagonal matrices of degree ν and νβν, while ν ββνν₯νβν and νββνβννν are arbitrary. For ν΄,ν΅ββν ν» the matrices ν and ν in (1.9) may be replaced by ν and ν β respectively, but then ν·1 and ν·2 represent any nonsingular real diagonal matrices. Lemma 1.12 Let ν΄ν΅,ν΅ν΅ββν ν» be star-ordered as ν΄ν΅β€βν΅ν΅. Then ν΄ν΅β€νΏν΅ν΅ if and only if νΎ ν΄ν΅ =νΎ ν΅ν΅ , Where νΎ (.) denotes the number of negative eigenvalues of a given bimatrix. Proof Case (i) Let ν ν΄ν΅ = ν ν΅ν΅ that is, ν ν΄1 = ν ν΅1 and ν ν΄2 = ν ν΅2 . The result is trivial. Case (ii) Let ν ν΄ν΅ < ν ν΅ν΅ that is, ν ν΄1 <ν ν΅1 and ν ν΄2 < ν ν΅2 Lemma (1.1) ensures that if ν΄ν΅β€βν΅ν΅, then ν΅ν΅βν΄ν΅= ν΅1βͺν΅2 β(ν΄1βͺν΄2) = ν΅1βν΄1 βͺ ν΅2βν΄2 = ν1 ν·11 0 0 ν·12 ν1ββν1 ν·11 00 0 ν1β βͺ ν2 ν·21 0 0 ν·22 ν2ββν2 ν·21 00 0 ν2β
4. On Some Partial Orderings for Bimatrices
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=(ν1βͺν2) ν·11βͺν·12 0 0 ν·12βͺν·22 ν1ββͺν2β β ν1βͺν2 ν·11βͺν·21 0 0 0 ν1ββͺν2β =νν΅ ν·ν΅1 0 0 ν·ν΅2 νν΅ ββνν΅ ν·ν΅1 0 0 0 νν΅ β ν΅ν΅βν΄ν΅=νν΅ 0 0 0 ν·ν΅2 νν΅ β Hence it is seen that the order ν΄ν΅β€νΏν΅ν΅ is equivalent to the non-negative definiteness of ν·ν΅2, that is, νΎ ν·2 =0.Consequently, the result follows by noting that νΎ ν΄ν΅ =νΎ ν·ν΅1 and νΎ ν΅ν΅ =νΎ ν·ν΅1 +νΎ ν·ν΅2 .
II. Star Partial Ordering
Theorem (3) of Baksalary and Pukel sheim [3] asserts that, for any A,B ββν β₯ , A β€βBβΊ A2β€βB2 βν΄ ν΅=ν΅ ν΄ (2.1) This result is revisited here with the emphasis laid on the question which from among four implications comprised in (2.1) continues to be valid for bimatrices not necessarily being bihermitian non negative definite. Theorem2.1 Let ν΄ν΅ββν νΈν and ν΅ν΅ββννν.Then ν΄ν΅β€βν΅ν΅βν΄ν΅ 2β€βν΅ν΅ 2 and ν΄ν΅ν΅ν΅=ν΅ν΅ν΄ν΅ (2.2) Proof Since ν΄ν΅=ν΄1βͺν΄2ββν νΈνβΊν΄ν΅ν΄ν΅ β =ν΄ν΅ β ν΄ν΅ That is, ν΄1ν΄1β =ν΄1β ν΄1 and ν΄2ν΄2β =ν΄2β ν΄2 Now, ν΄ν΅ 2ν΄ν΅ β =ν΄12 ν΄1β βͺν΄22ν΄2β =ν΄1 ν΄1ν΄1β βͺν΄2 ν΄2ν΄2β =ν΄1βͺν΄2 ν΄ν΅ 2ν΄ν΅ β =ν΄ν΅ Also, ν΄ν΅ β ν΄ν΅ 2=ν΄1β ν΄12 βͺν΄1β ν΄12 = ν΄1β ν΄1 ν΄1βͺ ν΄2+ ν΄2 =ν΄1βͺν΄2 ν΄ν΅ β ν΄ν΅ 2=ν΄ν΅ βν΄ν΅ 2ν΄ν΅ β =ν΄ν΅ β ν΄ν΅ 2 And ν΄ν΅ 2 β = ν΄12 βͺν΄22 β = ν΄1ν΄1 β βͺ ν΄2ν΄2 β =ν΄1β ν΄1β βͺν΄2β ν΄2β = ν΄1β βͺν΄2β 2 ν΄ν΅ 2 β = ν΄ν΅ β 2 Consequently, in view of (1.3), ν΄ν΅ν΅ν΅=ν΄1ν΅1βͺν΄2ν΅2 = ν΄12 ν΄1β ν΅1βͺν΄22ν΄2β ν΅2 =ν΄12 ν΄1β ν΄1βͺν΄22ν΄2β ν΄2
5. On Some Partial Orderings for Bimatrices
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ν΄ν΅ν΅ν΅=ν΄ν΅ 2 And ν΅ν΅ν΄ν΅=ν΅1ν΄1βͺν΅2ν΄2 =ν΅1ν΄1β ν΄12 βͺν΅2ν΄2β ν΄22 =ν΅1ν΄1β ν΄12 βͺν΄2ν΄2β ν΄22 ν΅ν΅ν΄ν΅=ν΄ν΅ 2 βν΄ν΅ν΅ν΅=ν΅ν΅ν΄ν΅=ν΄ν΅ 2 Moreover, ν΄ν΅ 2 β ν΅ν΅ 2= ν΄12 βͺν΄22 β ν΅12βͺν΅22 = ν΄12 β ν΅12βͺ ν΄22 β ν΅22 = ν΄12 β ν΄12 βͺ ν΄22 β ν΄22 = ν΄12 βͺν΄22 β ν΄12 βͺν΄22 ν΄ν΅ 2 β ν΅ν΅ 2= ν΄ν΅ 2 β ν΄ν΅ 2 and ν΅ν΅ 2 ν΄ν΅ 2 β =ν΅12 ν΄12 β βͺν΅22 ν΄22 β =ν΅1 ν΄1 ν΄1β 2βͺν΅2 ν΄2 ν΄2β 2 =ν΄12 ν΄12 β βͺν΄22 ν΄22 β ν΅22 ν΄ν΅ 2 β =ν΄ν΅ 2 ν΄ν΅ 2 β βΉν΄ν΅ 2β€βν΅ν΅ 2 Note2.2 Implication 2.2 is not reversible. Example2.3 Consider the bimatrices, ν΄ν΅= 1 10 0 βͺ 2 20 0 and ν΅ν΅= 1 11 β1 βͺ 2 22 β2 In which the order ν΄ν΅β€βν΅ν΅ does not entail either of the conditions ν΄ν΅ 2β€βν΅ν΅ 2, ν΄ν΅ ν΅ν΅=ν΅ν΅ ν΄ν΅. On the otherhand, if ν΄ν΅= 1 00 0 βͺ 2 00 0 and ν΅ν΅= 0 11 0 βͺ 0 22 0 then ν΄ν΅ 2 β€βν΅ν΅ 2, but ν΄ν΅ βν΄ν΅β ν΄ν΅ βν΅ν΅ and ν΄ν΅ ν΅ν΅β ν΅ν΅ ν΄ν΅. This showing that even for bihermitian matrices the star order between ν΄ν΅ 2 ννν ν΅ν΅ 2 and does not entail the star order between ν΄ν΅ and ν΅ν΅ and the commutativity of these bimatrices which are the other two implications contained in (2.1). It is pointed out that the two conditions on the right-hand side of (2.2) are insufficient for ν΄ν΅β€βν΅ν΅. When there is no restriction on ν΄ν΅, a similar conclusion is obtained in the case of combining the two orders ν΄ν΅β€βν΅ν΅ and ν΄ν΅ 2β€βν΅ν΅ 2.The bimatrices, ν΄ν΅= 0 10 0 βͺ 0 20 0 and ν΅ν΅= 0 11 0 βͺ 0 22 0 and their squares are star ordered, but ν΄ν΅ ν΅ν΅β ν΅ν΅ ν΄ν΅. However, the combination of the order ν΄ν΅β€βν΅ν΅ with the commutativity condition appears sufficient for ν΄ν΅ 2 β€βν΅ν΅ 2 for all quadratic bimatrices. Theorem2.4 Let ν΄ν΅,ν΅ν΅ββνν₯ν. Then ν΄ν΅β€βν΅ν΅ and ν΄ν΅ ν΅ν΅=ν΅ν΅ ν΄ν΅βΉν΄ν΅ 2 β€βν΅ν΅ 2
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Proof On account of (1.2), it follows that if ν΄ν΅β€βν΅ν΅ and ν΄ν΅ ν΅ν΅=ν΅ν΅ ν΄ν΅ then, ν΄ν΅ 2 βν΅ν΅ 2= ν΄12 βͺν΄22 β ν΅12βͺν΅22 = ν΄12 ββͺ ν΄22 β ν΅12βͺν΅22 = ν΄12 βν΅12βͺ ν΄22 βν΅22 =ν΄1β ν΄1β ν΄1 ν΅1βͺν΄2β ν΄2βν΄2 ν΅2 = ν΄1β 2 ν΄1 ν΅1βͺ ν΄2β 2ν΄2 ν΅2 =ν΄1 β ν΄1β ν΅1 ν΄1βͺν΄2β ν΄2βν΅2 ν΄2 = ν΄12 βν΄12 βͺ ν΄22 βν΄22 ν΄ν΅ 2 βν΅ν΅ 2= ν΄ν΅ 2 βν΄ν΅ 2 and ν΅ν΅ 2 ν΄ν΅ 2 β= ν΅12βͺν΅22 ν΄12 βͺν΄22 β =ν΅12 ν΄12 ββͺν΅22 ν΄22 β =ν΅1 ν΅1ν΄1 β ν΄1β βͺν΅2 ν΅2ν΄2 β ν΄2β =ν΅1 ν΄1ν΄1 β ν΄1 ββͺν΅2 ν΄2ν΄2 β ν΄2 β =ν΄1 ν΅1ν΄1 β ν΄1 ββͺν΄2 ν΅2ν΄2 β ν΄2 β =ν΄1 ν΄1ν΄1 β ν΄1 ββͺν΄2 ν΄2ν΄2 β ν΄2 β =ν΄12 ν΄1ν΄1 ββͺν΄22 ν΄2ν΄2 β =ν΄12 ν΄12 ββͺν΄22 ν΄22 β ν΅ν΅ 2 ν΄ν΅ 2 β=ν΄ν΅ 2 ν΄ν΅ 2 β
III. Minus Partial Ordering
Baksalary and Pukelsheim [3, Theorem 2] showed that for ,ν΅ββν β₯ , the following three implications hold. ν΄β€βν΅ and ν΄2β€βν΅2 βΉ ν΄ν΅=ν΅ν΄ (3.1) ν΄β€βν΅ and ν΄ν΅=ν΅ν΄ βΉ ν΄2β€βν΅2 (3.2) ν΄2β€βν΅2 and ν΄ν΅=ν΅ν΄ βΉ ν΄β€β ν΅ (3.3) Now,we extend this implications for bimatrices also by the following theorems. Theorem 3.1 For any ν΄ν΅,ν΅ν΅ββνν₯ν if ν΄ν΅β€β ν΅ν΅ and ν΄ν΅ν΅ν΅=ν΅ν΅ν΄ν΅ then ν΄ν΅ 2β€βν΅ν΅ 2 Proof First notice that, ν΄ν΅β€β ν΅ν΅ and ν΄ν΅ν΅ν΅=ν΅ν΅ν΄ν΅ (3.4) βΉν΄ν΅ν΅ν΅=ν΄1ν΅1βͺν΄2ν΅2=ν΄12 βͺν΄22=ν΅1ν΄1βͺν΅2ν΄2=ν΅ν΅ν΄ν΅ (3.5) On account of 1.7, it follows that, ν΄ν΅ν΅ν΅=ν΄1ν΅1βͺν΄2ν΅2 =ν΄1 ν΅1β ν΄1 ν΅1βͺν΄2 ν΅2β ν΄2ν΅2 =ν΄1 ν΅1β ν΅1 ν΄1βͺν΄2 ν΅2β ν΅2 ν΄2 =ν΄1ν΄1βͺν΄2ν΄2
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ν΅ν΅ β ν΄ν΅ ν΅ν΅ β ν΄ν΅ β =νν΅ νΌν΅ν 0βν ν΅β 0 νΌν΅ν β ν ν΅ 0 0 νν΅ β =νν΅ νΌν΅ν β ν ν΅ βν ν΅β ν ν΅β ν ν΅ νν΅ β (3.10) Since the bimatrix ν΅ν΅ β ν΅ν΅ =ν΅ν΅ν΅ν΅ β represents the orthogonal projector onto β ν΅ν΅ =β νν΅ , it may be expressed as νν΅νν΅ β. Consequently, in view of (3.10) ν΅ν΅ β ν΅ν΅βν΅ν΅ β ν΄ν΅ ν΅ν΅ β ν΄ν΅ β =νν΅ 0 ν ν΅ ν ν΅β νΌν΅(νβν) βν ν΅β ν ν΅ νν΅ β (3.11) On the account of (3.9), equality (3.11) shows that supplementing the minus order ν΄ν΅β€βν΅ν΅ by Lowner order ν΄ν΅ 2β€νΏν΅ν΅ 2 forces to be 0. Then the bimatrix ν΅ν΅ characterized in lemma (1.11) takes the form described in lemma (1.1), thus leading to the conclusion that ν΄ν΅β€βν΅ν΅ REFERENCES [1] Jerzy.K. Baksalary, Jan Hauke, Xiaoji Liu, Sanyang Liu, βRelationships between partial orders of matrices and their powersβ Linear Algebra and its Applications 379 (2004) 277-287. [2] J.K. Baksalary, S.K. Mitra, βLeft-star and right-star partial orderingsβ, Linear Algebra Applications, 149 (1991) 73- 89. [3] Jerzy.K. Baksalary, Oskar Haria Baksalary, Xiaoji Liu, βFurther properties of the star, left-star, minus partial orderingsβ Linear Algebra and its Applications 375 (2003) 83-94. [4] J.K. Baksalary, F. Pukelshiom, G.P.H. Styan, βsome properties of matrix partial orderingsβ, Linear Algebra Applications, 119 (1989) 57-85. [5] Jerzy.K. Baksalary, Sujit Kumar Mitra, βLeft-star and right-star and partial orderingsβ. Elsevier Science Publishing Co.,Inc.,1991 (73-89). [6] M.P. Drazin, βNatural structures on semi groups with involution Bull. Amer. Hath. Soc. 84 (1978) 139-141. [7] R.E.Hartwig, βHow to partially order regular elementsβ, Math. Japan.25 (1980) 1-13. [8] R.E. Hartwig, G.P.H. Styan, βon some characterizations of the star partial ordering for matrices and rank subtractivityβ, Linear Algebra Applications 82 (1986) 145-161. [9] K.S.S. Nambooripal, βThe natural partial order on a regular semi groupβ Proc. Edinburgh Math. Soc. 23 (1980) (249- 260). [10] Ramesh.G,Anbarasi.N, β On inverses and Generalized inverses of Bimatricesβ, International Journal of Research in Engineering and Technology, Vol.2, Issue 8, Aug 2014,PP(77-90)