Applied Mathematics
Vol.08 No.05(2017), Article ID:76280,8 pages
10.4236/am.2017.85050
Mixed-Type Reverse Order Laws for Generalized Inverses over Hilbert Space
Haiyan Zhang, Fengling Lu
College of Mathematics and Satistics, Shangqiu Normal University, Shangqiu, China
Copyright © 2017 by authors and Scientific Research Publishing Inc.
This work is licensed under the Creative Commons Attribution International License (CC BY 4.0).
http://creativecommons.org/licenses/by/4.0/
Received: April 4, 2017; Accepted: May 19, 2017; Published: May 22, 2017
ABSTRACT
In this paper, by using a block-operator matrix technique, we study mixed-type reverse order laws for {1,3}-, {1,2,3}- and {1,3,4}-generalized inverses over Hilbert spaces. It is shown that and when the ranges of are closed. Moreover, a new equivalent condition of is given.
Keywords:
{1,2,3}-Reverse, {1,3,4}-Reverse, Reverse Order Law, Block-Operator Matrix
1. Introduction
The reverse order law of generalized inverses plays an important role in theoretic research and numerical computations in many areas, including the singular matrix problem and optimization problem. They have attracted considerable attention since the middle 1960s, and many interesting results have been studied, see [1] - [10] .
For convenience, we firstly introduce some notations. Let H and K be infinite dimensional Hilbert spaces and be the set of all bounded linear operators from H to K and abbreviate to if . For an operator , and are the null space and the range of A, respectively. Denote by A* the adjoint of A. Recall that has a Moore-Penrose inverse if there exists an operator satisfies the following four equations, which is said to be the Moore-Penrose conditions:
If one exists, the Moore-Penrose inverse of A is unique and it is denoted by A+. And let denote the set of all operator which satisfy equations from among the above Moore-Penrose equations. Such G will be called a -inverse of A and will be denoted by . evidently, when A has closed range.
For the Moore-Penrose inverse, Greville [2] gave the necessary and sufficient conditions for on matrix algebra, this result was extended to bounded operators on Hilbert space by Izumino [4] . Subsequently, some researcher discussed the reverse order laws of other type generalized inverses, such
as [5] [6] [8] [10] . The mixed-type reverse-order
laws for AB like and were considered in [3] [4] when A and B are matrices. Motivated by this, Wang et al. [7] studied the mixed-type reverse-order laws for . Yang and Liu [9] gave the
equivalent condition of , by using
the extremal ranks of generalized Schur complements, when A and B are matrices. The mixed-type reverse order laws of were discussed on operator space over Hilbert space [5] .
In this article, we study the mixed-type reverse order laws of , and over infinite Hilbert space by using a block-operator matrix technique. For given A, B, it is shown that
and
when the ranges of A, B, AB are closed. We generalized the results from [7] and [9] to the case of bounded linear operators on Hilbert spaces. Moreover, a new
equivalent condition of is given.
2. Main Results
To obtain our main results, we begin with some notations and lemmas. Let with closed range. It is well known that A has the following matrix decomposition
(2.1)
where is invertible. Also, has the form
(2.2)
The {1,2,3}- and {1,3,4}-inverse has also similarly matrix form.
Lemma 1 ( [5] ). Let have closed range. Then
,
and
Let , and with closed ranges. For convenience, denote by
,
and
then
,
and
.
Under these space decomposition, we get two useful representations of operators and .
Lemma 2 ( [9] [10] ). Let , such that and are closed.
If , the following statements hold,
(1) When , A and B have the matrix form as follows, respectively,
(2.3)
(2.4)
where , , are invertible and is surjective.
(2) When ,
(2.5)
(2.6)
where , are invertible and is surjective.
Theorem 3. Let , such that and are closed. Then
.
Proof If , then , the result holds. So assume that . Next, we divide the proof into two cases.
Case 1. .
In this case, A, B have matrix forms (2.3) and (2.4), respectively. This implies that
(2.7)
Using Lemma 1, we get
(2.8)
and
(2.9)
where are arbitrary. Combining formulae (2.7) with (2.8), it is easy to get
Using Lemma 1 again, we have
(2.10)
where are arbitrary. By direct computation, it is clearly from (2.8) and (2.10) that
(2.11)
where , . Thus, by the arbitrariness of , it follows from fromulae (2.9) and (2.11) that
holds.
Case 2 . Obviously, . Consequently, and . By Lemma 2, have matrix forms (2.5) and (2.6), respectively. This follows that
(2.12)
By Lemma 1, we get
(2.13)
and
(2.14)
where are arbitrary. Combining formulae (2.12) with (2.13),
Again from Lemma 1,
where are arbitrary. By direct computation, it is clearly that
(2.15)
Thus, from fromulae (2.14) and (2.15), it is clear that
also holds in this case. The proof is completed.
From the relationship of {1,2,3}-inverse and {1,2,4}-inverse, we can obtain the following result without proof.
Corollary 4. Let , such that and are closed. Then
.
Similar to the proof of Theorem 3, we also can get the following result.
Theorem 5. Let , such that and are closed. Then
.
In [5] , the author gave a necessary and sufficient condition of
. Next, we give a new equivalent condition
of the mixed-type reverse order law for .
Theorem 6. Let , such that and are closed. If , the following statements are equivalent,
(1) ;
(2)
Proof We divide the proof into two cases.
Case 1. . Using Lemma 2, A, B have matrix forms (2.3) and (2.4), respectively. The operator AB has the matrix decomposition (2.7). Then
(2.16)
and
(2.17)
by direct computation from (2.3) and (2.4). Therefore, comparing (2.16) with (2.17), it is natural that if and only if . So if and only if since is invertilbe.
On the other hand, it follows from Lemma 1 that
(2.18)
and
(2.19)
where are arbitrary.
Combining formulae (2.7) with (2.18), it is easy to get
.
Using Lemma 1 again, we have
(2.20)
where are arbitrary. By direct computation, it is clearly from (2.18) and (2.20) that
(2.21)
Comparing (2.21) with (2.19), we have
if and only if , that is, . Therefore, if and only if .
Case 2 . Then A, B have matrix forms (2.5) and (2.6), respectively. By similarly discussing to case 1 and case 2 in the proof of Theorem 3.2, it is easy
to get that and al-
ways hold in this case.
So the proof is completed.
Acknowledgements
This subject is supported by NSF of China (No. 11501345) and the Natural Science Basic Research Plan of Henan Province (No. 152300410221).
Cite this paper
Zhang, H.Y. and Lu, F.L. (2017) Mixed-Type Reverse Order Laws for Generalized Inverses over Hilbert Space. Applied Mathematics, 8, 637-644. https://doi.org/10.4236/am.2017.85050
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