Abstract
In this paper, we introduce a new generalized inverse called -CCE inverse which presents a generalization of the CCE inverse in Minkowski space by using the -core-EP decomposition and the Minkowski inverse. We first show the existence and the uniqueness of the generalized inverse. Then, a number of basic properties and diverse characterizations are derived for the -CCE inverse as well as its limit and integral expressions. Additionally, applications of the -CCE inverse are given in solving a system of linear equations. Applying the generalized inverse, we introduce a binary relation based on the -CCE inverse.
MSC:
15A09; 15A24; 15A29
1. Introduction
Generalized inverses are studied in many branches of mathematical field: matrix theory, operator theory, -algebras, rings, etc. Additionally, generalized inverses turn out to be a powerful tool in many applications such as Markov chains, differential equations, difference equations, electrical networks, optimal control, and so on.
Penrose [1] earliest defined the Moore–Penrose inverse using four matrix equations in 1955. Then, a wave of research on generalized inverses has begun. In 1958, Drazin [2] introduced the Drazin inverse with spectral properties in associative rings and semigroups. The Drazin inverse of a group matrix is also known as its group inverse [3]. Using the Moore–Penrose inverse and the Drazin inverse, Malik and Thome [4] defined the DMP inverse in 2014. The core inverse was firstly proposed by Baksalary and Trenkler [5] in 2010 as an alternative to the group inverse. Manjunatha Prasad and Mohana [6] then extended the core inverse in 2014 by introducing the core-EP inverse. In 2016, Wang [7] introduced the core-EP decomposition, which plays a crucial role in the investigation of generalized inverses. In 2018, Mehdipour introduced the CMP inverse by applying the Moore–Penrose inverse and the Drazin inverse. In 2020, Zuo [8] defined the CCE inverse based on the core-EP decomposition.
In studying polarized hight, Renardy [9] investigated the singular value decomposition in Minkowski space in order to quickly verify that a Mueller matrix can map the forward light cone into itself. Subsequently, the Minkowski inverse in Minkowski space was established by Meenakshi [10], who also gave a condition for a Mueller matrix to have a singular value decomposition in Minkowski space according to its Minkowski inverse. Recently, Wang and Liu defined the -core inverse [11], the -core-EP inverse [12], the -WG inverse [13] and the -WG° inverse [14] in Minkowski space, which can be regarded as extensions of the core inverse [5], the core-EP inverse [6], the weak group inverse [15] and the m-weak group inverse [16], respectively. In 2023, Zuo [17] promoted the DMP inverse to Minkowski space; we call it the -DMP inverse afterward.
Inspired by the study of the CCE inverse and the generalized inverses in Minkowski space, the intention of this paper is to introduce a new generalized inverse in Minkowski space, called the -CCE inverse, and discuss its properties, characterizations, representations and applications.
2. Preliminaries
In this paper, we denote the Minkowski space by , which is an n-dimensional complex vector space with the metric matrix diag , where denotes the identity matrix of order . It is easy to check that and . We define that for (including for ), where represents the set of all real matrices.
Let , be the sets of all complex n-dimensional vectors and complex matrices. * means the conjugate transpose of a matrix. The symbols , , and denote the conjugate transpose, range, null space, and rank, respectively, of . Let . If , we call X an outer inverse of A, which is denoted by . If an outer inverse X of A satisfies and , then X is called the outer inverse with the prescribed range and null space , which is denoted by . The Minkowski adjoint of matrix A is denoted by , and it is defined as , where and are Minkowski metric matrices with orders m and n, respectively. For a matrix A, the index of A is the smallest non-negative integer k such that , which is denoted as . Notice that if and only if A is invertible. For subspaces and satisfying their direct sum as , i.e., , the projector onto along is indicated by .
The Moore–Penrose inverse denoted by of is the unique matrix satisfying the following matrix equations [1]
The Drazin inverse denoted by of with is the unique matrix satisfying the following matrix equations [2]
When , is called the group inverse of A denoted by [3].
The DMP inverse denoted by of with is the unique matrix satisfying the following matrix equations [4]
notice that and represents the dual DMP (or MPD) inverse of A.
The core-EP inverse denoted by of with is the unique matrix satisfying the following matrix equations [6].
notice that .
The CMP inverse denoted by of is the unique matrix satisfying the following matrix equations [18]
notice that .
The CCE inverse denoted by of is the unique matrix satisfying the following matrix equations [8]
notice that . Evidently, the core-EP inverse underpins the CCE inverse by supplying essential properties and acting as its building block, whereas the CCE inverse constitutes an extension of the core-EP inverse. From Theorem 3.9 of [8], we obtain that if and only if , where .
The Minkowski inverse denoted by of with and in Minkowski space is the unique matrix satisfying the following matrix equations [10]
The -DMP inverse denoted by of with and in Minkowski space is the unique matrix satisfying the following matrix equations [17]
notice that and represents the dual -DMP (or -MPD) inverse of A.
The -core inverse denoted by of with and in Minkowski space is the unique matrix satisfying the following matrix equations [11]
The -core-EP inverse denoted by of with and in Minkowski space is the unique matrix satisfying the following matrix equations [12]
notice that .
Lemma 1
([17]). Let . Then, the following conditions are equivalent:
- (1)
- exists;
- (2)
- ;
- (3)
- .
Lemma 2
([10]). Let with . Then,
- (1)
- and ;
- (2)
- ;
- (3)
- .
Lemma 3
([19]). Let with , . Then,
- (1)
- and ;
- (2)
- .
Lemma 4
([20]). Let with and . Then,
- (1)
- and ;
- (2)
- .
Lemma 5
([21]). If X is an outer inverse of A, then
Lemma 6
([19]). Let . Let L and M be complementary subspaces of , i.e., .Then,
- (1)
- ;
- (2)
- .
Lemma 7
([22]). Every matrix with has a Hartwig–Spindelböck decomposition:
where is a unitary matrix, diag is a diagonal matrix, the elements on the diagonal being the singular values of the matrix A, , and and satisfy .
Lemma 8
([17]). Let be given by (1), let , and let the partition of the Minkowski metric matrix be
where , and . If Δ and are nonsingular, then
The -core-EP inverse of A is given as [14]
3. The -CCE Inverse in Minkowski Space
This section defines a new generalized inverse named -CCE inverse in Minkowski space. In order to do this, we recall the -core-EP decomposition firstly. Then, we consider a system of equations.
Lemma 9
([12]). Let with and . Then, matrix A has an -core-EP decomposition , and it has the following matrix form
where , , , and is unitary. Furthermore,
where and hold the form as Lemma 8, is nonsingular, , and is nilpotent such that . In addition, the -core-EP decomposition of matrix A is unique and , .
Let with , and having the decomposition as Lemma 9. Let . Consider the following system of equations.
Theorem 1.
The system (2) has a unique solution .
Proof.
Definition 1.
Let with , and . The -CCE inverse of A in Minkowski space, which is denoted by , is defined as
Example 1.
Let
Then, , and . Also,
This shows that -CCE inverse is different from some known generalized inverse.
4. Characterizations and a Canonical Form of the -CEE Inverse
More characterizations for the Moore–Penrose inverse, the Drazin inverse, the DMP inverse, the CCE inverse, the Minkowski inverse, the -core-EP inverse and the -core inverse can be found in [23,24,25,26], and we now present characterizations for the -CCE inverse.
Theorem 2.
Let with , and . Then,
- (1)
- ;
- (2)
- ;
- (3)
- .
Proof.
on the other hand, we can obtain from
In addition, since G denoted as a Minkowski metric matrice is nonsingular, it follows that
It is obvious that
which implies
As a consequence, we obtain
Due to , we deduce that
In conclusion, we obtain . □
(1) From Lemmas 4 and 5, we know
(2) According to Lemma 2, we know that
Using Lemma 6, we obtain that
which implies
From Lemma 5, we have that
This implies
Furthermore,
Hence, we obtain .
- (3)
- On the one hand, according to item (1) and item (2), we obtain
Theorem 3.
Let with , and . Then,
- (1)
- ;
- (2)
- .
Proof.
It is obvious that
which shows that
Hence, we can infer that
furthermore,
So, . In conclusion, . □
(1) Using Theorem 2, we possess
According to Theorem 2(2), we know
Hence, we know .
- (2)
- According to Theorem 2(1), we know
Theorem 4.
Let with , and . Then,
- (1)
- is an outer inverse of A;
- (2)
- is a reflexive g-inverse of ;
- (3)
- , .
Proof.
In conclusion, we observe that is a reflexive g-inverse of .
Hence, we obtain the results. □
(1) This is evident.
- (2)
- Using the properties of and , we can compute directly that
- (3)
- It is obvious that
Theorem 5.
Let with , and . Then, presents a unique solution of
Proof.
Theorem 6.
Let with , and . Then, the following statements are equivalent:
- (1)
- ;
- (2)
- , ;
- (3)
- , ;
- (4)
- , .
Proof.
where the last equality follows from Lemmas 4 and 6.
using Lemma 6, we obtain
Applying to , we have
This finishes the proof. □
(1) ⇒ (2). It is easily obtained by (2) and Theorem 2.
- (2) ⇒ (3).
- Post-multiplying by , we earn
- (3) ⇒ (4).
- We know is an idempotent from . It follows that
- (4) ⇒ (1).
- Since Theorem 3, we obtain
Theorem 7.
Let with , and . Then, the following statements are equivalent:
- (1)
- ;
- (2)
- , , ;
- (3)
- , , ;
- (4)
- , , .
Proof.
According to Definition 1, we realize
(3) ⇒ (4). Applying to , we gain
(4) ⇒ (1). It is easily obtained by Theorem 1.
This completes the proof. □
(1) ⇒ (2). It is obvious by Theorem 4.
- (2) ⇒ (3).
- Applying and to , we gain
Theorem 8.
Let with , and . Then,
- (1)
- ;
- (2)
- .
Proof.
From item (1), we know . □
(1) The result is easily obtained by Lemma 9.
- (2)
- It is obvious that
Theorem 9.
Let with , and . Then,
- (1)
- ;
- (2)
- ;
- (3)
- ;
- (4)
- ;
- (5)
- ;
- (6)
- .
Proof.
(2) According to the properties of and , we have
(3) According to the properties of and , we obtain
(4) According to the properties of and , we know
(5) Pre-multiplying by , we earn
It follows that from . The converse is obvious.
The converse is obvious. □
From Lemmas 3 and 4, we acquire
Using Lemma 6, we attain
It can be easily obtained that
Hence, we secure the following proof.
- (1)
- According to the properties of and , we know
- (6)
- Because and the fact that , we realize
Theorem 10.
Proof.
5. Representations
In this section, we present some representations for -CCE inverse.
Lemma 10
([27]). Let , and . If exists, then
Lemma 11
([28]). Let . Then,
Lemma 12
([19]). Let with . If is a full-rank decomposition and are also full-rank decompositions. Then,
- (1)
- is invertible;
- (2)
- ;
- (3)
- .
Lemma 13
([29]). Let be a rank factorization of rank r and . Then,
Theorem 11.
Let with and . If A has a full-rank decomposition as Lemma 12, then
Proof.
Let . We must verify that X satisfies , and
. Then,
Thus, we obtain the result. □
Theorem 12.
Let with and . If A has a full-rank decomposition as Lemma 12, then
where , .
Proof.
Let , . Then, and . According to Theorem 11, we know
It follows from that
This finishes the proof. □
Theorem 13.
Let with , and . If A has a full-rank decomposition as Lemma 12, then
where , .
Proof.
Using Lemma 13, Theorem 12 and the fact that , we have
This finishes the proof. □
Example 2.
Let
Then, and . In addition,
Example 3.
Let us test the matrix A given in Example 1. Then, , and
where and have been shown in Example 1.
Theorem 14.
Let with , and . Let A be the full-rank decomposition as Lemma 12. Then,
where , , .
Proof.
It is clear that
which implies
In addition, since is of full column rank, it follows that
This shows exists by Lemma 1. Also, From Lemma 1 and Theorem 2, we have
According to Lemma 6, we obtain
Using Lemma 11 and Theorem 13, we attain
where . This finishes the proof. □
Theorem 15.
Let with , and . Then,
- (1)
- ;
- (2)
- ;
- (3)
- ;
- (4)
- .
Proof.
(2) Let , . Then, we can obtain the result through a similar way.
We have in Theorem 2 already. Combining with Lemmas 10 and 11(2), we have the following proof.
- (1)
- Let , . Then,
- (3)
- Let , . Then, we can obtain the result.
- (4)
- Let , . Then, we can obtain the result. □
Example 4.
Consider the matrix A given in Example 1. Then, ,
It is easy to check that , where has been shown in Example 1.
6. Applications
Theorem 16.
Let with , and . Then, the general solution to the linear system
is , where is arbitrary.
Proof.
Theorem 17.
Let with , and . Suppose and . If , then the restricted matrix equation
has the unique solution .
Proof.
Theorem 18.
Let with , and . Let and be of full column rank such that and . Then, the bordered matrix
is nonsingular, and its inverse is given by
Proof.
From , we realize . Since
it follows that .
Let
then
Hence, . □
Theorem 19.
Let with , and . Let and be as Theorem 18, and be as Theorem 17. Then, the unique solution of (5) is given by , where
where denotes the j-th column of D and and mean to substitute the i-th column of A and C by and 0, respectively.
7. A Binary Relation Based on the -CCE Inverse
In this section, we study the binary relation for the -CCE inverse.
Definition 2.
Let with , and . We consider that A is below B under the relation if
The relation is denoted by A B.
It is easy to know that the binary relation is reflexive. According to the following examples, we observe it is neither anti-symmetric nor transitive.
Example 5.
Consider a matrix as follows. Let B be the transpose of the matrix A.
It is easy to check that
By computing, we have
i.e., and . But . This means the relation is not anti-symmetric.
Example 6.
Consider the matrices
Then, we have
What is more, we have
i.e., , , But , which means we cannot obtain . Thus, the relation is not transitive. Above all, we know is not a matrix partial order.
8. Conclusions
This paper introduces the -CCE inverse, which is an extension of the CCE inverse in Minkowski space. Some of its properties, characterizations, representations, and applications in solving a system of linear equations are also shown in this paper. In addition, we prove that the -CCE ordering is not a matrix partial ordering. Because of the wide range of research fields and application backgrounds of generalized inverses, we convince that further explorations of the -CCE inverse will receive more attention and interest from researchers. Some possibilities for further research are given as follows:
- Further properties, characterizations and representations of the -CCE inverse.
- We can further generalize the -CCE inverse to tensors.
- The perturbation analysis and iterative methods for the -CCE inverse will be two topics worth studying.
- It is equally interesting to discuss the -CCE inverse for rectangular matrices.
Author Contributions
Methodology, X.L.; formal analysis, X.T.; writing—original draft, X.T.; writing—review & editing, X.L.; Funding acquisition, X.L. All authors have read and agreed to the published version of the manuscript.
Funding
The authors were supported by the National Natural Science Foundation of China (Grant Number 12061015) and Guangxi Natural Science Foundation (Grant Number 2024GXNSFAA010503).
Data Availability Statement
The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.
Conflicts of Interest
The authors declare no conflicts of interest.
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