Left and Right Inverse Eigenpairs Problem for -Hermitian Matrices
Hindawi Publishing Corporation
Journal of Applied Mathematics
Volume 2013, Article ID 230408, 6 pages
http://dx.doi.org/10.1155/2013/230408
Research Article
Left and Right Inverse Eigenpairs Problem
for π
-Hermitian Matrices
Fan-Liang Li,1 Xi-Yan Hu,2 and Lei Zhang2
1
Institute of Mathematics and Physics, School of Sciences, Central South University of Forestry and Technology,
Changsha 410004, China
2
College of Mathematics and Econometrics, Hunan University, Changsha 410082, China
Correspondence should be addressed to Fan-Liang Li;
Received 6 December 2012; Accepted 20 March 2013
Academic Editor: Panayiotis J. Psarrakos
Copyright Β© 2013 Fan-Liang Li et al. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Left and right inverse eigenpairs problem for π
-hermitian matrices and its optimal approximate problem are considered. Based on
the special properties of π
-hermitian matrices, the equivalent problem is obtained. Combining a new inner product of matrices,
the necessary and sufficient conditions for the solvability of the problem and its general solutions are derived. Furthermore, the
optimal approximate solution and a calculation procedure to obtain the optimal approximate solution are provided.
1. Introduction
Throughout this paper we use some notations as follows. Let
πΆπΓπ be the set of all π Γ π complex matrices, ππΆπΓπ , π»πΆπΓπ ,
ππ»πΆπΓπ denote the set of all π Γ π unitary matrices, hermitian
matrices, skew-hermitian matrices, respectively. Let π΄, π΄π»,
and π΄+ be the conjugate, conjugate transpose, and the MoorePenrose generalized inverse of π΄, respectively. For π΄, π΅ β
πΆπΓπ , β¨π΄, π΅β© = re(tr(π΅π»π΄)), where re(tr(π΅π»π΄)) denotes the
real part of tr(π΅π»π΄), the inner product of matrices π΄ and π΅.
The induced matrix norm is called Frobenius norm. That is,
βπ΄β = β¨π΄, π΄β©1/2 = (tr(π΄π»π΄))1/2 .
Left and right inverse eigenpairs problem is a special
inverse eigenvalue problem. That is, giving partial left and
right eigenpairs (eigenvalue and corresponding eigenvector),
(π π , π₯π ), π = 1, . . . , β; (ππ , π¦π ), π = 1, . . . , π, a special matrix set
π, finding a matrix π΄ β π such that
π΄π₯π = π π π₯π ,
π = 1, . . . , β,
π¦ππ π΄ = ππ π¦ππ ,
π = 1, . . . , π.
eigenpairs problem. For example, we studied the left and
right inverse eigenpairs problem of skew-centrosymmetric
matrices and generalized centrosymmetric matrices, respectively [5, 6]. Based on the special properties of left and right
eigenpairs of these matrices, we derived the solvability conditions of the problem and its general solutions. In this paper,
combining the special properties of π
-hermitian matrices and
a new inner product of matrices, we first obtain the equivalent
problem, then derive the necessary and sufficient conditions
for the solvability of the problem and its general solutions.
Hill and Waters [7] introduced the following matrices.
Definition 1. Let π
be a fixed product of disjoint transpositions, and let πΎ be the associated permutation matrix, that is,
πΎ = πΎπ» = πΎ, πΎ2 = πΌπ , a matrix π΄ β πΆπΓπ is said to be π
hermitian matrices (skew π
-hermitian matrices) if and only
if πππ = ππ(π)π(π) (πππ = βππ(π)π(π) ), π, π = 1, . . . , π. We denote the
set of π
-hermitian matrices (skew π
-hermitian matrices) by
πΎπ»πΆπΓπ (ππΎπ»πΆπΓπ ).
(1)
This problem, which usually arises in perturbation analysis
of matrix eigenvalues and in recursive matters, has profound
application background [1β6]. When the matrix set π is
different, it is easy to obtain different left and right inverse
From Definition 1, it is easy to see that hermitian matrices
and perhermitian matrices are special cases of π
-hermitian
matrices, with π(π) = π and π(π) = π β π + 1, respectively.
Hermitian matrices and perhermitian matrices, which are
one of twelve symmetry patterns of matrices [8], are applied
in engineering, statistics, and so on [9, 10].
2
Journal of Applied Mathematics
From Definition 1, it is also easy to prove the following
conclusions.
(1) π΄ β πΎπ»πΆπΓπ if and only if π΄ = πΎπ΄π»πΎ.
(2) π΄ β ππΎπ»πΆπΓπ if and only if π΄ = βπΎπ΄π»πΎ.
(3) If πΎ is a fixed permutation matrix, then πΎπ»πΆπΓπ and
ππΎπ»πΆπΓπ are the closed linear subspaces of πΆπΓπ and
satisfy
πΆπΓπ = πΎπ»πΆπΓπ β¨ ππΎπ»πΆπΓπ .
(2)
The notation π1 β π2 stands for the orthogonal direct sum of
linear subspace π1 and π2 .
Μ β
(4) π΄ β πΎπ»πΆπΓπ if and only if there is a matrix π΄
Μ = πΎπ΄.
π»πΆπΓπ such that π΄
Μ β
(5) π΄ β ππΎπ»πΆπΓπ if and only if there is a matrix π΄
πΓπ
Μ = πΎπ΄.
ππ»πΆ such that π΄
Proof. (1) From Definition 1, if π΄ = (πππ ) β πΎπ»πΆπΓπ , then
πππ = ππ(π)π(π) , this implies π΄ = πΎπ΄π»πΎ, for πΎπ΄π»πΎ = (ππ(π)π(π) ).
(2) With the same method, we can prove (2). So, the proof
is omitted.
(3)
(a) For any π΄ β πΆπΓπ , there exist π΄ 1 β πΎπ»πΆπΓπ ,
π΄ 2 β ππΎπ»πΆπΓπ such that
π΄ = π΄ 1 + π΄ 2,
(3)
where π΄ 1 = (1/2)(A + πΎπ΄π»πΎ), π΄ 2 = (1/2)(π΄ β
πΎπ΄π»πΎ).
(b) If there exist another π΄1 β πΎπ»πΆπΓπ , π΄2 β
ππΎπ»πΆπΓπ such that
π΄ = π΄1 + π΄2 ,
(4)
(5)
Multiplying (5) on the left and on the right by
πΎ, respectively, and according to (1) and (2), we
obtain
π΄ 1 β π΄1 = π΄ 2 β π΄2 .
Problem 2. Giving π β πΆπΓβ , Ξ = diag(π 1 , . . . , π β ) β πΆβΓβ ;
π β πΆπΓπ , Ξ = diag(π1 , . . . , ππ ) β πΆπΓπ , find π΄ β πΎπ»πΆπΓπ such
that
π΄π = πΞ,
ππ π΄ = Ξππ .
Μ β ππΈ such that
Problem 3. Giving π΅ β πΆπΓπ , find π΄
σ΅©σ΅©
Μσ΅©σ΅©σ΅©σ΅© = min βπ΅ β π΄β ,
σ΅©σ΅©π΅ β π΄
σ΅© βπ΄βππΈ
σ΅©
(8)
(9)
where ππΈ is the solution set of Problem 2.
This paper is organized as follows. In Section 2, we first
obtain the equivalent problem with the properties of πΎπ»πΆπΓπ
and then derive the solvability conditions of Problem 2 and its
general solutionβs expression. In Section 3, we first attest the
existence and uniqueness theorem of Problem 3 then present
the unique approximation solution. Finally, we provide a
calculation procedure to compute the unique approximation
solution and numerical experiment to illustrate the results
obtained in this paper correction.
2. Solvability Conditions of Problem 2
We first discuss the properties of πΎπ»πΆπΓπ
Lemma 4. Denoting π = πΎπΈπΎπΊπΈ, and πΈ β π»πΆπΓπ , one has
the following conclusions.
(3)-(4) yields
π΄ 1 β π΄1 = β (π΄ 2 β π΄2 ) .
In this paper, we suppose that πΎ is a fixed permutation
matrix and assume (π π , π₯π ), π = 1, . . . , β, be right eigenpairs
of π΄; (ππ , π¦π ), π = 1, . . . , π, be left eigenpairs of π΄. If we let
π = (π₯1 , . . . , π₯β ) β πΆπΓβ , Ξ = diag (π 1 , . . . , π β ) β πΆβΓβ ;
π = (π¦1 , . . . , π¦π ) β πΆπΓπ , Ξ = diag(π1 , . . . , ππ ) β πΆπΓπ , then the
problems studied in this paper can be described as follows.
(6)
Combining (5) and (6) gives π΄ 1 = π΄1 , π΄ 2 = π΄2 .
(c) For any π΄ 1 β πΎπ»πΆπΓπ , π΄ 2 β ππΎπ»πΆπΓπ , we have
π»
β¨π΄ 1 , π΄ 2 β© = re (tr (π΄π»
2 π΄ 1 )) = re (tr (πΎπ΄ 2 πΎπΎπ΄ 1 πΎ))
= re (tr (βπ΄π»
2 π΄ 1 )) = β β¨π΄ 1 , π΄ 2 β© .
(7)
This implies β¨π΄ 1 , π΄ 2 β© = 0. Combining (a), (b),
and (c) gives (3).
Μπ» = π΄
Μ β π»πΆπΓπ .
Μ = πΎπ΄, if π΄ β πΎπ»πΆπΓπ , then π΄
(4) Let π΄
π»
πΓn
π»
Μ β π»πΆ , then π΄ = πΎπ΄
Μ and πΎπ΄ πΎ = πΎπ΄
Μπ»πΎπΎ =
Μ =π΄
If π΄
Μ = π΄ β (...truncated)