In this paper, we present an iterative algorithm to solve a generalized coupled Sylvester – conjugate matrix equations over Hamiltonian matrices. When the considered systems of matrix equations are consistent, it is proven that the solution can be obtained within finite iterative steps for any arbitrary initial generalized Hamiltonian matrices in the absence of round off errors. Two numerical examples are given to illustrate the effectiveness of the proposed method.
In this paper, the symbols and represent the transpose, conjugate, conjugate transpose and the trace of a matrix A, respectively. denote the real part of number represents the set of all complex matrices. The matrix is a generalized Hamiltonian matrix if where J is an skew – Hermitian matrix, that is, . Also, the set of all generalized Hamiltonian matrices is denoted by , that is, where J is an skew – Hermitian matrix.
Consider the generalized coupled Sylvester – conjugate matrix equations
where , and are given matrices, while are matrices to be determined. Matrix equations are often encountered in many areas of computational mathematics, control and system theory. By using the Kronecker product, the exact solutions can be readily obtained. However, this direct method may suffer from computing problems with the dimensions increasing. In Chang et al. (2010), the expression of – conjugate solution about by matrix decompositions is given. Trench (2004) defined R- conjugate matrix and defined - conjugate matrix in Trench (2005). Trench (2004) studied the system of linear equations for R– conjugate matrices and for – conjugate matrices in Trench (2005), respectively, where are known column vectors. Li (2017) constructed a finite iterative method to solve the generalized Hamiltonian coupled Sylvester matrix equations with conjugate transpose. Dehghan and Hajarian (2011a) introduced the reflexive solution of the Sylvester matrix equation . Madiseh and Dehghan (2014) extended the concept of generalized solution sets to the interval generalized Sylvester matrix equation . The general expressions of the -symmetric and -skew symmetric solutions were given in Dehghan and Hajarian (2011b). (Dehghan and Hajarian, 2010, 2012a, 2012b) obtained the solutions, the generalized bisymmetric solutions, the generalized centro-symmetric and central anti-symmetric solutions by extending the CGNE iterative method and GI method. Hajarian (2014) solved general coupled matrix equations by using the matrix form of the CGS method. Beik and Salkuyeh (2017) developed a robust iterative algorithm to find the least-squares -orthogonal symmetric and skew-symmetric solution sets of generalized coupled matrix equations. Beik and Moghadam (2014) proposed an algorithm to solve a class of general coupled linear matrix equations over the complex number field and the optimal approximately generalized reflexive and anti-reflexive solution groups are derived. Beik and Salkuyeh (2013) presented an iterative algorithm for solving coupled Sylvester-transpose matrix over generalized centro-symmetric matrices and derived the optimal approximate generalized centro-symmetric solution. Salkuyeh and Beik (2015) dealt with the problem of finding the minimum norm least-squares solution of a quite general class of coupled linear matrix equations defined over the complex number field and present the convergence properties of the algorithm.
This paper is organized as follows. First, in section 2, we introduce some definitions, lemmas and theorem that will be needed to develop this work. In section 3, we propose iterative methods to obtain numerical solutions to the generalized coupled Sylvester – conjugate matrix equation (1) over Hamiltonian matrices. In section 4, two numerical examples are given to explore the simplicity and the neatness of the presented methods.
Preliminaries
The following definition, lemmas and theorem will be used to develop the proposed work.
Definition 1. Inner product (Zhang, 2004): A real inner product space is a vector space V over the real field ℝ together with an inner product, that is, with a map
Satisfying the following three axioms for all vectors and all scalars
Symmetry:.
Linearity in the first argument .
Positive definiteness: > 0 for all .
The following theorem defines a real inner product on space over the field ℝ.
Theorem 1 (Wu et al., 2011): In the space over the field ℝ, an inner product can be defined as
The Frobenius norm of A is denoted by , that is, . The matrices are called orthogonal if
Lemma 1 (Li, 2017): For any , then where J is an skew – Hermitian matrix.
hold for integer . We will prove this conclusion by induction. The case of has been proven in Step 1. Now, we assume that (7) and (8) hold for the aim is to show
and
First, we prove the following
and
By Lemma 3 and Lemma 4 we have
and
This implies that (11) and (12) holds.
By Lemma 3 and Lemma 4 it follows that
and
Repeating (13) and (14), one can easily obtain for certain and
and
This implies that (7) and (8) holds for .
Thus, from Steps (1) and (2), the conclusion holds by the principle of induction.
Lemma 6: Suppose that the system of matrix equations (1) is consistent and let , be its generalized Hamiltonian solutions. Then for any initial matrices , . We have
where the sequences and are generated by Algorithm 1 for .
Proof: We apply mathematical induction.
For , from Algorithm 1 one has
In view that are solutions of the generalized coupled Sylvester – conjugate matrix equation (1), it is easy to obtain from the above relation
This implies that (15) holds for .
Now, assume that (15) holds for . That is
Then we have to prove that the conclusion holds for .
Since
We get
In view that are solutions of the generalized coupled Sylvester – conjugate matrix equation (1), it is easy to obtain from the above relation
This implies that (15) holds for . Hence, relation (15) holds by the principle of induction.
Remark: Lemma 6 implies that if there exist a positive number j such that but, then the system of matrix equation (1) is inconsistent.
With the above two lemmas, one has the following theorem that guarantees the algorithm will converge after a finite number of iterations.
Theorem 2: If the system of matrix equation (1) is consistent, then a solution can be obtained within a finite number of iteration steps in the absence of round off errors by using Algorithm 1 for any arbitrary initial generalized Hamiltonian matrices , .
Proof:
Let ,
Suppose that for , we get from Lemma 6 and remark. Then we can compute , by Algorithm 1. Also, from Lemma 5, we have
So, the set of is an orthogonal basis of the linear space of dimension where }
This implies that
, that is, are the generalized Hamiltonian solution of system of matrix equation (1).
Numerical example
In this section, we present two numerical examples to illustrate the application of our proposed algorithm.
Example 1: Consider the generalized coupled Sylvester – conjugate matrix equations
The obtained results are presented in Figure 1, where
From Figure 1, it is clear that the error is becoming smaller and approaches zero as iteration number k increases. This indicates that the proposed algorithm is effective and convergent.
The residual and the relative error versus k (iteration number).
Example 2: Consider the generalized coupled Sylvester – conjugate matrix equations
The obtained results are presented in Figure 2, where
From Figure 2, it is clear that the error is becoming smaller and approaches zero as iteration number k increases. This indicates that the proposed algorithm is convergent.
The residual versus k (iteration number).
Conclusions
An iterative algorithm for solving the generalized coupled Sylvester – conjugate matrix equation (1) over Hamiltonian matrices is presented. We have proven that the iterative algorithms always converge to the solution for any arbitrary initial generalized Hamiltonian matrices . We stated and proved some lemmas and theorems where the solutions are obtained. The obtained results show that the methods are very neat and efficient. The proposed method is illustrated by numerical examples. The examples we tested using MATLAB to verify our theoretical results.’
Footnotes
Acknowledgements
The authors would like to express their heartfelt thanks to the editor and anonymous referees for their useful comments.
Declaration of conflicting interest
The authors declare that there is no conflict of interest.
Funding
This research received no specific grant from any funding agency in the public, commercial, or not-for-profit sectors.
ORCID iD
Ahmed ME Bayoumi
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