Abstract
This paper investigates new solution sets for the Yang–Baxter-like (YB-like) matrix equation involving constant entries or rational functional entries over complex numbers. Towards this aim, first, we introduce and characterize an essential class of generalized outer inverses (termed as -inverses) of a matrix, which commute with it. This class of -inverses is defined based on resolving appropriate matrix equations and inner inverses. In general, solutions to such matrix equations represent optimization problems and require the minimization of corresponding matrix norms. We decided to analytically extend the obtained results to the derivation of explicit formulae for solving the YB-like matrix equation. Furthermore, algorithms for computing the solutions are developed corresponding to the suggested methods in some computer algebra systems. The main features of the proposed approach are highlighted and illustrated by numerical experiments.
Keywords:
Yang–Baxter-like matrix equation; outer inverse; Moore–Penrose inverse; idempotent matrices; computer algebra MSC:
15A09; 15A24; 68W30
1. Introduction and Literature Review
Given a square matrix A; we are concerned about finding the unknown matrix X which fulfills the matrix equation
This equation is called the Yang–Baxter-like (YB-like, for short) matrix equation. If A is singular (resp. nonsingular), we call (1) the singular (resp. nonsingular) YB-like matrix equation. Furthermore, if the entries of A are constants (resp. multivariate rational functions with coefficients) over the field of complex numbers , then Equation (1) is said to be the constant (resp. rational) YB-like matrix equation.
Equation (1) possesses a similar format to the famous Yang–Baxter equation, first introduced by Yang [1] in 1967 and then by Baxter [2] independently in 1972, in the field of statistical mechanics. The classic Yang–Baxter equation has been a hot research area in science and engineering applications, closely related to various mathematical subjects, such as knot theory [3], braid groups [4], statistical mechanics [5], and quantum research [6]. So, it is necessary to find partial or general solutions of (1) from the viewpoint of matrix theory. The YB-like matrix equation is identifiable as the star-triangle-like equation in statistical mechanics ([7], [Part III]) and [8].
Notice that (1) is a quadratic matrix equation with at least two (trivial) solutions, and , but its nonlinearity makes it challenging to solve: the problem of calculating a nontrivial solution requires solving a system of quadratic equations with variables, which is a complex task.
Many direct methods have recently been constructed to find several classes of solutions to (1) and most of them are based on the structure of A; see, e.g., [9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24] and references therein. To illustrate it further, all solutions were investigated in [9] for the matrix such that , where u and v are n-dimensional vectors. In [10], commuting solutions have been located for the situation where A has some particular Jordan forms. Solutions to (1) for some types of Jordan canonical form of A were suggested in [11]. All commuting solutions for a diagonalizable matrix and non-commuting solutions for a Householder matrix are discovered in [12]. All solutions to (1) were found in [13,14,15] when A is an idempotent and a rank-one matrix, respectively. Spectral solutions were studied in [16,17]. It was shown in [18] that any semisimple eigenvalue of a matrix A gives rise to infinitely many solutions. This result was extended in [19] to the matrix A having a non-semisimple eigenvalue with at least Jordan block. The complete solution set can be attained from [20,21,22] for the matrix A of rank two. All the commuting solutions were found for the matrix , where P and Q are two matrices of full column rank and det(. All solutions that commute with A were identified in [23] provided . In [24], all the solutions were observed for A such that and has a rank equal to one or two.
However, by increasing the dimension of the input matrix A, direct methods cannot be used in practice for solving the Equation (1) due to considerable cost in both time and space requirements. This observation has led some analysts to suggest and rely on numerical methods to discover solutions. Such solutions were obtained in [25] using the classic Brouwer fixed point theorem for a nonsingular quasi-stochastic matrix A such that is stochastic. The authors of [26] proposed iterative methods for calculating commuting solutions via the mean ergodic theorem for the diagonalizable matrix A. Some iterative methods have been presented in [27] for an arbitrary matrix A. An iterative method based on the Hermitian and skew-Hermitian splitting of the matrix A was introduced in [28].
Zeroing neural network (ZNN) dynamical system approach has been exploited in solving the time-varying Yang–Baxter matrix equation , where the given and the unknown are real time-varying square matrices. Various ZNN dynamical systems were proposed in [29,30,31].
The rank optimization problem related to the YB matrix equation was considered in [32].
After all, the computation of the solutions to the rational YB-like equation in symbolic implementation has not been investigated so far. The symbolic calculation is an essential area of computer algebra and scientific computing. Moreover, there has not been any efficient algorithm for solving YB-like equation if the matrix A is arbitrary and with entries given as rational functions with an arbitrary number of variables with coefficients over complex numbers. This paper contributes to resolving these issues. Recall that in [33], the authors have developed effective formulae for calculating infinitely many solutions using finite-precision arithmetic. Nevertheless, those methods do not perform well when A is an ill-conditioned or a matrix with multivariate rational functional entries.
The global organization is based on the following sections. Main generalized inverses and corresponding matrix equations that define them are surveyed in Section 2. Some notations, notions, and motivations are also introduced and discussed therein. Next, in Section 3, we provide a theoretical basis for determining a specific variety of {2,5} generalized inverses in terms of inner inverses. The required inner inverses can be generated as solutions of an appropriate couple of linear matrix equations. Then in Section 4, we set up a correlation between the explicit solutions to the YB-like matrix equation and {2,5}-inverses of some appropriate matrix. Algorithms for solving the matrix Equation (1) are developed based on introduced results in the previous section. These algorithms are easily implementable in the programming language MATHEMATICA. Numerical experiments are given in Section 5 to support the claims given in this work. Finally, the conclusions of this paper will be drawn in Section 6.
2. Preliminaries and Motivation
Let be the set of multivariate rational functions with complex coefficients in the unknown variables . As usual, (resp. ) denotes the set of matrices over (resp. over ), while (resp. ) stands for the subset of (resp. of ) which includes matrices of rank r. The symbol I stands for the identity matrix of an appropriate order. By , rank(M), and we mean the conjugate-transpose, the rank, the range and the null space of a matrix , respectively. The index of a square matrix M is defined as ind(. The following matrix equations
define different classes of generalized inverses of a nonzero matrix ; see [34,35,36,37,38]. In fact, if , then a complex matrix X is called a -inverse of M if X satisfies equation , for each . The notation stands for the set of all -inverses if . Any matrix from is always denoted by . Particularly, , called the Moore–Penrose inverse of M, which always exists and is unique. Furthermore, there is a unique inverse of a square matrix M called the Drazin inverse, and is its label. The Drazin inverse coincides with the group inverse if ind.
A selected which fulfils as well as will be termed as . A matrix is said to be an outer generalized inverse of M if it belongs to . The fundamental result that describes the existence of outer inverse with prescribed range and null space of is restated in Lemma 1.
Lemma 1
([34], Theorem 2.14). Let , let T be a subspace of of dimension , and let S be a subspace of of dimension . Then, M has a -inverse(or outer inverse)X such that and if and only if , in which case X is unique and is denoted by .
There exist a number of representations for outer inverses with determined range and null space in the literature [39,40,41,42,43,44,45]. Now we revisit an important lemma for determining .
Lemma 2
([42]). For the same , and S as in Lemma 1, the -inverse exists if and only if there exists such that , and . Furthermore,
Our main intention in this paper is the development of algorithms for finding the solutions to the rational YB-like matrix equation . These algorithms are based on newly derived solution representations to the desired matrix equation. Towards this aim, we generate a unique approach with the help of the class of {2,5}-inverses of a nonzero matrix , for appropriate . Such matrix inverses will be named as commuting outer inverses of M. Developed algorithms are based on solving a suitable system of linear matrix equations under exact rank conditions. The underlying matrix equations are considered as minimization problems and can be solved using various methods. We use exact and numerical solutions to these matrix equations in a computer algebra system. In further steps, commuting outer inverses of M are used to define a relevant projector P and two appropriate choices of a matrix B. Each choice of B is finally used in defining a collection of solutions to the YB-like matrix equation. This central goal is developed through the following primary outcomes of this research.
- (a)
- Several equivalent characterizations and initiated representations of are given.
- (b)
- Necessary and sufficient conditions when becomes are investigated.
- (c)
- Proposed results about the requirement as well as computational procedures for obtaining are applied with the aim of deriving explicit formulae to solve the YB-like Equations (1).
- (d)
- Algorithms for solving YB–like matrix equation with constant entries or entries given as rational functions with several variables are presented.
- (e)
- Implementation of the proposed algorithms in the MATHEMATICA computer Algebra system is developed, and illustrative examples are executed.
3. Existence, Characterizations and Representations of {2,5}-Inverses
This section will examine some crucial properties of {2,5}-inverses with the prescribed range and null space of a square matrix M.
The forthcoming Theorem 1 and Corollary 1 provide equivalent conditions for the existence and representations of as well as . Domain of obtained representations are complex square matrices and utilize solutions of a particular pair of linear matrix equations. Consequently, some new relationships are established between solutions to the linear matrix equations and obtaining {2,5}-inverses with determined range and null space.
Theorem 1.
Let , , and .
- (a)
- The subsequent statements are mutually equivalent:
- (i)
- exists;
- (ii)
- There exists satisfying , and ;
- (iii)
- There exist satisfying , and ;
- (iv)
- There exist and satisfying , , and ;
- (v)
- There exist and satisfying , , and ;
- (vi)
- , and , for some (equivalently every) inner inverse .
- (b)
- If an arbitrary of the statements (i)–(vi) is valid, thenfor arbitrary and an arbitrary satisfying , and .
Proof.
(a) (i) ⇒ (ii): Let be such that , , and . Then there exists which determines X by . In addition, E and F fulfill the conditions and , for some , . This further implies
(ii) ⇒ (iii): This implication is clear.
(iii) ⇒ (vi): Assume the existence of such that and . In that case
It further yields
Hence,
Similarly we can prove .
(vi) ⇒ (i): If (vi) holds, one obtains
Thus, Similarly, Therefore, by ([41], [Theorem 6]) and ([43], [Corollary 2.5]), exists and . Notice that
(ii) ⇒ (iv): Suppose existence of satisfying and . Such assumptions initiate
which confirms (iv).
(iv) ⇔ (v): This equivalence is evident.
(v) ⇒ (i): Let the equations , and are fulfilled for some and . Consider . Such conditions initiate
which gives . Also
Now , which implies . In addition, based on , it follows . Therefore, .
(b) From the proof of (i)⇒ (ii), we can see that for . Next from the proof of (vi)⇒(i), if , and , for some (equivalently every) , then exists. Since the statements (ii) and (vi) are equivalent, therefore , and imply . All these facts imply
Hence, the proof is completed. □
The following corollary is obtained as a consequence of Theorem 1.
Corollary 1.
Let .
- (a)
- The subsequent statements are mutually equivalent:
- (i)
- exists;
- (ii)
- There exists satisfying ;
- (iii)
- There exist satisfying ;
- (iv)
- There exist satisfying , and ;
- (v)
- There exist satisfying , and ;
- (vi)
- , for some (equivalently every) .
- (b)
- If an arbitrary of the statements(i)–(vi)is valid, thenfor arbitrary fixed and an arbitrary such that the matrix equations are solvable.
Theorem 6 in [41] and Corollary 2.5 in [43] can be used for finding . In the following Theorem 2, we examine specific conditions on ranges and null spaces which provide commutativity of with M.
Theorem 2.
Let , , and be such that exists, i.e., . Then the following statements are equivalent:
- (i)
- ;
- (ii)
- , and ;
- (iii)
- , and ;
- (iv)
- , and ;
- (v)
- , and ;
- (vi)
- , and .
Proof.
(i) ⇒ (ii): Using and in conjunction with (i), we obtain (ii).
(ii) ⇒ (iii): This implication is obvious.
(iii) ⇒ (i): Using and , we obtain as well . Since and , then , for some and . Therefore,
and similarly . Thus
(i) ⇔ (iv): Since and are idempotents, then
(iv) ⇔ (v): This implication is obvious.
(iv) ⇒ (vi): Using from ([41], [Theorem 6]) or ([43], [Corollary 2.5]), this part is evident.
(vi) ⇒ (ii): Based on it is noticed from ([41], [Theorem 3]) and ([43], [Corollary 2.1]) that
for some . Similarly, from Theorem 4 in [41] and Corollary 2.3 in [43],
for some . From Equations (2) and (3), it is concluded that . A further consequence of the inclusion is
In the same way, yields . □
The upcoming result can be verified using Theorem 2.
Corollary 2.
Let be such that exists. Then the following statements are equivalent:
- (i)
- ;
- (ii)
- ;
- (iii)
- , and ;
- (iv)
- , and ;
- (v)
- ;
- (vi)
- , and .
4. Commuting Outer Inverse-Based Solutions to Yang–Baxter-like Matrix Equation
Following the intention of the previous section, in this section we investigate the possibility of solving the YB-like equation using obtained results about -inverses. Before proceeding, we require results included in Lemma 3.
Lemma 3.
Proof.
Corollary 3.
Proof.
We define an infinite collection of complex numbers by
At this point, we prove the following existence result for the YB-like matrix equation corresponding to an arbitrary square matrix A.
Theorem 3.
Let be a given arbitrary matrix. Consider a nonzero matrix , for any . Consider a nonzero matrix , where . Suppose , and be such that any of the following assumptions(A1)–(A2)holds:
- (A1) One of the statements (i)–(vi) of part (a) in Theorem 1 is true;
- (A2) One of statements (i)–(vi) of part (a) in Theorem 2 is true and exists.
Proof.
Suppose the assumption (A1) holds. Then it follows from part (a)(i) of Theorem 1 that exists. Using the facts and , it is clear that P is an idempotent and commutes with M and hence with A. The first statement is verified. For the given choice of B, it follows from [33] (Lemma 4.1) that the matrix B satisfies the conditions in (5). So by Lemma 3 (resp. Corollary 3), the second assertion follows. The remaining proof under the assumption (A2) is immediate. □
In the same way, we can present the following conclusion.
Corollary 4.
Let be arbitrary. Consider a nonzero matrix , where . Suppose be such that any of the following assumptions (AS1)–(AS2) holds:
- (AS1) One of the statements (i)–(vi) of part (a) in Corollary 1 is true;
- (AS2) One of statements (i)–(vi) of part(a)in Corollary 2 is true, provided exists.
Remark 1.
Let the matrix B be suggested by Theorem 3 or Corollary 4. Then,
- (a)
- X represented by (4) will be an infinite family of solutions of the singular YB-like Equation (1), since the involved matrix Y is arbitrary. In addition, the entries of X consist of ’s if Y is taken in the form . According to (4.1) in singular case, unevaluated symbols ’s are incorporated into the elements of the resulting matrix X.
- (b)
Theorem 1 provides not only criteria for the existence of , but also a method for detecting such an inverse. More precisely, the problem of determining {2,5}-inverse X of M satisfying and reduces to finding a solution U to the system or under specific constraints. Then -inverse X of M satisfying and can be obtained as . On the other hand, Theorem 3 is based on the usage of to spot the solutions of the equation for a suitable matrix .
Remark 2.
Since , it is clear from Corollary 2.5. in [43] that the existence of requires . This condition will be exploited when making a selection of matrices E and F.
Thus, we can state the Algorithm 1 for generating solutions to (1), according to the results presented in Theorems 1 and 3.
| Algorithm 1 Solving the singular (resp. nonsingular) YB-like matrix Equation (1) using Theorem 1 in conjunction with Theorem 3. |
Require: The matrix
|
We recall that Theorem 6 in [41] and Corollary 2.5 in [43] deliver two frameworks for computing , in case . The first approach is based on the direct computation of and the second one is enabled in which is calculated by solving a matrix equation or . On the other hand, Theorem 2 investigates equivalent axioms when becomes .
These consequences in association with Theorem 3 make it possible to present the Algorithm 2 for producing solutions to (1).
| Algorithm 2 Solving the singular (resp. nonsingular) YB-like matrix Equation (1) using Theorem 2 in conjunction with Theorem 3. |
Require: The matrix .
|
5. Implementation Details and Illustrative Experiments
This section aims to describe main implementation details and develop test examples to verify the practical applicability of theoretical findings discussed in the above sections. The key point in implementing Algorithm 1 is to solve , required in Step 3:. On the other hand, the solution based on an arbitrary inner inverse in Step 4: of Algorithm 2 can be calculated by ([41], [Theorem 6]) or ([43], [Corollary 2.5]) using the following steps 3.1: and 3.2:
- 3.1:
- Solve the matrix equation with respect to unknown matrix .
- 3.2:
- Compute .
So, the implementation Algorithm 2 is based on the matrix equation .
Step 3: in Algorithm 1 and Step 3: in Algorithm 2 in the constant matrix environment can be considered as the minimization problems
where is the time and is unknown state variables matrix. The Gradient Neural Network (GNN) evolution from [41] based on the goal function (8) is defined by the following GNN dynamical flow:
The implementation of Step 3: in Algorithm 1 and Step 3: in Algorithm 2 in the general multivariate case was proposed in [43], and it is based on symbolic capabilities of programming package MATHEMATICA [46].
For a given matrix A and a suitable matrix B, the explicit formula (4) involves the computation of generalized inverses and . It is worth mentioning that the Moore–Penrose inverse of an arbitrary matrix can be evaluated in MATHEMATICA through the built-in function PseudoInverse, whose implementation is based on its singular value decomposition.
Example 1.
Let us consider three-variable singular rational YB-like Equation (1), where
This example is based on Algorithm 1 for the singular case, where . Furthermore, we take the following matrices E and F in conjunction with M:
Here the matrices E and F are generated according to the rank conditions The expression U = Table[Subscript[u,i,j], {i,4}, {j,4}] generates the matrix with unassigned symbols as entries. Let vars = Flatten[U]; then the general solution U is obtained using the MATHEMATICA command Solve[MEUFE==E, vars]//Simplify or Solve[FEUFM==F, vars]//Simplify and it is as follows:
Therefore it is justifiable to apply Theorem 1, which produces the output
Further, simple calculations confirm that
is idempotent and commutes with A. Since A is singular, X is given by (4); assuming , for the matrix , with . Then one calculates
Example 2
Let . The goal of this example is again to illustrate Algorithm 1 for the nonsingular case in the situation , where
with . For this choice of G, the solution to the system can be obtained similarly as in above example. As a confirmation, it is equal to
So, with the help of Corollary 1, we deduce
Therefore, the matrix
is an idempotent and commutes with A. Since A is nonsingular, let X be the singleton matrix of the form (7). If , then when . In this situation, simplifications give
It can be checked that X is a solution to the matrix Equation (1). Likewise, by putting is also a solution.
Example 3.
Let . We deal with the constant YB-like matrix equations, where the complex matrix is defined by
and is imaginary unit.
For a given n, here, it is easy to confirm that is nonsingular. We implemented the Algorithm 2 in machine precision arithmetic to spot the solution to Equation (1) in for the nonsingular case.
Let n be fixed. To illustrate the script, we take corresponding to the choice . In this example, G is taken as a singular matrix of index one commuting with M.
Since M is nonsingular, it is easy to verify that the declaration in Step 2 of the algorithm is satisfied. Consequently, by Lemma 2, exists. Notice that . This observation shows that the condition in Step4:of Algorithm 2 also holds.
Observe . Then by the representation (7), the required approximation can be located, with the choice . Here we use the expression est to measure the absolute error and to estimating the quality of .
The results are displayed in Table 1. According to data involved in the table, is a nontrivial solution because and are nonzero. From the value of est, it is straightforward that is a reliable estimation of the solution from the point of accuracy.
Table 1.
Frobenius-norm errors in Example 3.
The numerical reports and evidence in this section clearly show a good agreement with the theoretical aspects of the paper.
6. Conclusions
The Yang–Baxter-like matrix equation has been widely studied and utilized in numerous fields of mathematics and physics. This research presents a valuable application of -inverses in solving the Yang–Baxter matrix equation. In order to achieve this aim, we have described the set of -inverses (termed commuting outer inverses) with predefined image and kernel as auxiliary results. Then the application of the given approach in developing the solution structures for constant as well as rational YB-like matrix equations is pointed out. In this way, algorithms defined on rational matrices are constructed based on the correlation between the symbolic calculation of the aforementioned inverses and derived explicit solutions of the matrix equation. The algorithm based on any proposed formula can be implemented in some computer algebra systems. Implementing those computational procedures in symbolic form, in the form of exact arithmetic and double-precision arithmetic is also a concern. Thus, this paper has greatly extended the previous work of [33].
Finally, some numerical experiments are performed to manifest the superiority of the proposed methods.
The results obtained in this paper are another confirmation that generalized inverses are closely related to solving the Yang–Baxter matrix equation. It is logical to assume that generalized inverses can be used in many new ways in solving this complex problem. In addition, it can be expected that other classes of generalized inverses are also included at the basis of solutions to YB-like equations. One exciting area for research may be solving the minimization problem (8) instead of finding the exact solution to embedded matrix equations employing a symbolic programming package. In addition, the rank optimization problem could be solved in a number of different ways.
Author Contributions
Conceptualization: A.K.; Data curation: P.S.S. and G.S.; Formal analysis: A.K., D.M., P.S.S. and G.S.; Funding acquisition: L.A.K.; Investigation: A.K., D.M., P.S.S. and G.S.; Methodology: P.S.S.; Project administration, L.A.K.; Resources: L.A.K.; Software, A.K.; Supervision, P.S.S. and G.S.; Validation, D.M.; Writing—original draft, D.M.; Writing—review and editing, L.A.K. All authors have read and agreed to the published version of the manuscript.
Funding
This work was supported by the Ministry of Science and Higher Education of the Russian Federation (Grant No. 075-15-2022-1121).
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
Not applicable.
Acknowledgments
Ashim Kumar acknowledges the I. K. Gujral Punjab Technical University Jalandhar, Kapurthala for providing research support to him. Dijana Mosić and Predrag Stanimirović are supported from the Ministry of Education, Science and Technological Development, Republic of Serbia, Grants 451-03-68/2022-14/200124. Predrag Stanimirović is supported by the Science Fund of the Republic of Serbia, (No. 7750185, Quantitative Automata Models: Fundamental Problems and Applications-QUAM). We acknowledge that This work was supported by the Ministry of Science and Higher Education of the Russian Federation (Grant No. 075-15-2022-1121).
Conflicts of Interest
The authors declare no conflict of interest.
References
- Yang, C.N. Some exact results for the many-body problem in one dimension with repulsive delta-function interaction. Phys. Rev. Lett. 1967, 19, 1312–1315. [Google Scholar] [CrossRef]
- Baxter, R.J. Partition function of the eight-vertex lattice model. Ann. Phys. 1972, 70, 193–228. [Google Scholar] [CrossRef]
- Przytycki, J.H. Knot theory: From Fox 3-colorings of Links to Yang-Baxter Homology and Khovanov Homology. In Knots, Low-Dimensional Topology and Applications; Springer: Cham, Switzerland, 2019; Volume 284, pp. 115–145. [Google Scholar]
- Yang, C.N.; Ge, M.L. Braid Group, Knot Theory and Statistical Mechanics; World Scientific: Singapore, 1989. [Google Scholar]
- Vieira, R.S.; Lima-Santos, A. Solutions of the Yang-Baxter equation for (n + 1) (2n + 1)-vertex models using a differential approach. J. Stat. Mech. Theory Appl. 2021, 2021, 053103. [Google Scholar] [CrossRef]
- Tsuboi, Z. Quantum groups, Yang-Baxter maps and quasi-determinants. Nucl. Phys. B 2018, 926, 200–238. [Google Scholar] [CrossRef]
- McCoy, B.M. Advanced Statistical Mechanics; Oxford University Press: New York, NY, USA, 2009. [Google Scholar]
- Nichita, F.F. Nonlinear Equations, Quantum Groups and Duality Theorems: A Primer on the Yang–Baxter Equation; VDM: Saarbru¨cken, Germany, 2009. [Google Scholar]
- Ding, J.; Tian, H. Solving the Yang–Baxter-like matrix equation for a class of elementary matrices. Comp. Math. Appl. 2016, 72, 1541–1548. [Google Scholar] [CrossRef]
- Ding, J.; Zhang, C.; Rhee, N.H. Commuting solutions of the Yang–Baxter matrix equation. Appl. Math. Lett. 2015, 44, 1–4. [Google Scholar] [CrossRef]
- Ding, J.; Zhang, C.; Rhee, N.H. Further Solutions of a Yang–Baxter-like Matrix Equation. East Asian J. Appl. Math. 2013, 3, 352–362. [Google Scholar] [CrossRef]
- Dong, Q.; Ding, J. Complete commuting solutions of the Yang–Baxter-like matrix equation for diagonalizable matrices. Comput. Math. Appl. 2016, 72, 194–201. [Google Scholar] [CrossRef]
- Cibotarica, A.; Ding, J.; Kolibal, J.; Rhee, N. Solutions of the Yang–Baxter matrix equation for an idempotent. Numer. Algebra Control Optim. 2013, 3, 347–352. [Google Scholar] [CrossRef]
- Mansour, S.I.A.; Ding, J.; Huang, Q. Explicit solutions of the Yang–Baxter-like matrix equation for an idempotent matrix. Appl. Math. Lett. 2017, 63, 71–76. [Google Scholar] [CrossRef]
- Tian, H. All solutions of the Yang–Baxter-like matrix equation for rank-one matrices. Appl. Math. Lett. 2016, 51, 55–59. [Google Scholar] [CrossRef]
- Ding, J.; Rhee, N.H. Spectral solutions of the Yang–Baxter matrix equation. J. Math. Anal. Appl. 2013, 402, 567–573. [Google Scholar] [CrossRef]
- Zhou, D.; Chen, G.; Yu, G.; Zhong, J. On the projection-based commuting solutions of the Yang–Baxter matrix equation. Appl. Math. Lett. 2018, 79, 155–161. [Google Scholar] [CrossRef]
- Ding, J.; Zhang, C. On the structure of the spectral solutions of the Yang–Baxter matrix equation. Appl. Math. Lett. 2014, 35, 86–89. [Google Scholar] [CrossRef]
- Dong, Q. Projection-based commuting solutions of the Yang–Baxter matrix equation for non-semisimple eigenvalues. Appl. Math. Lett. 2017, 64, 231–234. [Google Scholar] [CrossRef]
- Zhou, D.; Chen, G.; Ding, J. On the Yang–Baxter-like matrix equation for rank-two matrices. Open Math. 2017, 15, 340–353. [Google Scholar] [CrossRef]
- Zhou, D.; Chen, G.; Ding, J. Solving the Yang–Baxter-like matrix equation for rank-two matrices. J. Comp. Appl. Math. 2017, 313, 142–151. [Google Scholar] [CrossRef]
- Yin, H.-H.; Wang, X.; Tang, X.-B.; Chen, L. On the commuting solutions to the Yang–Baxter-like Matrix Equation for Identity Matrix Minus Special Rank-two Matrices. Filomat 2018, 32, 4591–4609. [Google Scholar] [CrossRef]
- Zhou, D.; Chen, G.; Ding, J. Solving the Yang–Baxter-like matrix equation for nilpotent matrices of index three. Int. J. Comput. Math. 2018, 95, 303–315. [Google Scholar] [CrossRef]
- Zhou, D.; Ding, J. All Solutions of the Yang–Baxter-Like Matrix Equation for Nilpotent Matrices of Index Two. Complexity 2020, 2020, 2585602. [Google Scholar] [CrossRef]
- Ding, J.; Rhee, N.H. A Nontrivial Solution to a Stochastic Matrix Equation. East Asian J. Appl. Math. 2012, 2, 277–284. [Google Scholar] [CrossRef]
- Ding, J.; Rhee, N.H. Computing Solutions of the Yang–Baxter-like matrix equation for diagonalisable matrices. East Asian J. Appl. Math. 2015, 5, 75–84. [Google Scholar] [CrossRef]
- Kumar, A.; Cardoso, J.R. Iterative methods for finding commuting solutions of the Yang–Baxter-like matrix equation. Appl. Math. Comput. 2018, 333, 246–253. [Google Scholar] [CrossRef]
- Dehghan, M.; Shirilord, A. HSS-like method for solving complex nonlinear Yang–Baxter matrix equation. Eng. Comput. 2021, 37, 2345–2357. [Google Scholar] [CrossRef]
- Zhang, H.; Wan, L. Zeroing neural network methods for solving the Yang–Baxter-like matrix equation. Neurocomputing 2020, 383, 409–418. [Google Scholar] [CrossRef]
- Wendong, J.; Lin, C.-L.; Katsikis, V.N.; Mourtas, S.D.; Stanimirović, P.S.; Simos, T.E. Zeroing Neural Network Approaches Based on Direct and Indirect Methods for Solving the Yang–Baxter-like Matrix Equation. Mathematics 2022, 10, 1950. [Google Scholar] [CrossRef]
- Shi, T.; Tian, Y.; Sun, Z.; Liu, K.; Jin, L.; Yu, J. Noise-tolerant neural algorithm for online solving Yang–Baxter-type matrix equation in the presence of noises: A control-based method. Neurocomputing 2021, 424, 84–96. [Google Scholar] [CrossRef]
- Lifang, D.; Maolin, L.; Yonghong, S. Some Rank Formulas for the Yang–Baxter Matrix Equation AXA=XAX. Wuhan Univ. Nat. Sci. 2021, 26, 459–463. [Google Scholar]
- Kumar, A.; Cardoso, J.R.; Singh, G. Explicit solutions of the singular Yang–Baxter-like matrix equation and their numerical computation. Mediterr. J. Math. 2022, 19, 85. [Google Scholar] [CrossRef]
- Ben-Israel, A.; Greville, T.N.E. Generalized Inverses: Theory and Applications, 2nd ed.; Springer: New York, NY, USA, 2003. [Google Scholar]
- Golub, G.H.; Van Loan, C.F. Matrix Computations, 3rd ed.; Johns Hopkins University Press: Baltimore, ML, USA, 1996. [Google Scholar]
- Laub, A. Matrix Analysis for Scientists and Engineers; SIAM: Philadelphia, PA, USA, 2005. [Google Scholar]
- Lütkepohl, H. Handbook of Matrices; Wiley: New York, NY, USA, 1996. [Google Scholar]
- Mitra, S.K.; Bhimasankaram, P.; Malik, S.B. Matrix Partial Orders, Shorted Operators and Applications; World Scientific: Singapore, 2010. [Google Scholar]
- Mosić, D.; Stanimirović, P.S.; Sahoo, J.K.; Behera, R.; Katsikis, V.N. One-sided weighted outer inverses of tensors. J. Comput. Appl. Math. 2021, 388, 113293. [Google Scholar] [CrossRef]
- Sheng, X.; Chen, G. Full-rank representation of generalized inverse of and its applications. Comp. Math. Appl. 2007, 54, 1422–1430. [Google Scholar] [CrossRef] [Green Version]
- Stanimirović, P.S.; Ćirić, M.; Stojanović, I.; Gerontitis, D. Conditions for existence, representations, and computation of matrix generalized inverses. Complexity 2017, 2017, 6429725. [Google Scholar] [CrossRef] [Green Version]
- Chen, Y.L.; Tan, X.Y. Computing generalized inverses of matrices by iterative methods based on splittings of matrices. Appl. Math. Comput. 2005, 163, 309–325. [Google Scholar] [CrossRef]
- Stanimirović, P.S.; Ćirić, M.; Lastra, A.; Sendra, J.R.; Sendra, J. Representations and symbolic computation of generalized inverses over fields. Appl. Math. Comput. 2021, 406, 126287. [Google Scholar] [CrossRef]
- Stanimirović, P.S.; Pappas, D.; Katsikis, V.N.; Stanimirović, I.P. Full-rank representations of outer inverses based on the QR decomposition. Appl. Math. Comput. 2012, 218, 10321–10333. [Google Scholar] [CrossRef]
- Wei, Y. A characterization and representation of the generalized inverse and its applications. Linear Algebra Appl. 1998, 280, 87–96. [Google Scholar] [CrossRef] [Green Version]
- Trott, M. The Mathematica Guidebook for Numerics; Springer: New York, NY, USA, 2006. [Google Scholar]
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