Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 537520, 7 pages http://dx.doi.org/10.1155/2013/537520 Research Article Necessary and Sufficient Conditions for the Existence of a Positive Definite Solution for the Matrix Equation π πΏπ π΄ π + ∑π π=1 π π π΄ π = πΌ Naglaa M. El-Shazly Department of Mathematics, Facultyof Science, Menoufia University, Shebin El-Koom, Egypt Correspondence should be addressed to Naglaa M. El-Shazly; naglaamoh1@yahoo.com Received 19 December 2012; Revised 26 March 2013; Accepted 14 May 2013 Academic Editor: Theodore E. Simos Copyright © 2013 Naglaa M. El-Shazly. 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. π In this paper necessary and sufficient conditions for the matrix equation π + ∑π=1 π΄ππ ππΏπ π΄ π = πΌ to have a positive definite solution π are derived, where −1 < πΏπ < 0, πΌ is an π × π identity matrix, π΄ π are π × π nonsingular real matrices, and π is an odd positive integer. These conditions are used to propose some properties on the matrices π΄ π , π = 1, 2, . . . , π. Moreover, relations between the solution π and the matrices π΄ π are derived. denote by π(π΄), π(π΄), and βπ΄β the spectral radius of π΄, the eigenvalues of π΄, and the Euclidean norm of π΄, respectively. The notation π΄ > π΅ (π΄ ≥ π΅) indicates that π΄ − π΅ is positive definite (semidefinite). 1. Introduction Consider the nonlinear matrix equation π π + ∑ π΄ππ ππΏπ π΄ π = πΌ, π=1 −1 < πΏπ < 0, (1) where πΌ is an π × π identity matrix, π΄ π are π × π nonsingular real matrices, and π is an odd positive integer (π΄∗π stands for the conjugate transpose of the matrix π΄ π ). Several authors [1– 13] have studied the existence, the rate of convergence, as well as the necessary and sufficient conditions of the existence of positive definite solutions of similar kinds of nonlinear matrix equations. This paper is organized as follows. First, in Section 2, we introduce some notations, lemmas, and theorems that will be needed to develop this work. In Section 3, we present necessary and sufficient conditions for the existence of a positive definite solution of (1). In Section 4, some applications of the obtained results as well as relations between the solution π and the matrices π΄ π are given. 2. Preliminaries In this section, we present some notations, lemmas, and theorems that will be needed to develop this paper. We Lemma 1. Let πΈ and πΉ be two arbitrary compatible matrices. Then, π (πΈπ πΉ − πΉπ πΈ) ≤ π (πΈπ πΈ + πΉπ πΉ) . (2) The proof of this lemma is given in [14, Lemma 6]. Theorem 2 (Cholesky Decomposition). If πΊ is an π × π symmetric positive definite matrix, then there exists a triangular π × π matrix π with positive diagonal entries such that πΊ = ππ π. For proof, see [15, page 141]. Theorem 3 (C-S decomposition [15, page 77] and [16, page 11 π12 37]). If π is an orthogonal matrix where π = [ π π21 π22 ], then there exist orthogonal matrices π1 , π2 , π1 , π2 and diagonal matrices Γ ≥ 0, Σ ≥ 0 such that Γ −Σ π1 0 π 0 ][ ], π=[ 1 ][ 0 π2 Σ Γ 0 π2 where Γ2 + Σ2 = πΌ. (3) 2 Journal of Applied Mathematics 3. Necessary and Sufficient Conditions and (8) means that the columns of π π1 ( π2 ) .. . In this section, we derive both necessary and sufficient conditions for the existence of a positive definite solution of the nonlinear matrix equation (1). Theorem 4. The matrix equation (1) has a solution π (symmetric and positive definite) if and only if π΄ π , π = 1, 2, . . . , π, admit the following factorization: π π π=1 π=1 ∑ π΄ π = ∑ (ππ π) −πΏπ /2 ππ , (4) (11) ππ are orthonormal. Conversely, suppose that π΄ π , π = 1, 2, . . . , π have the decomposition (4). Set π = ππ π. Then π where π is a nonsingular square matrix and the columns of π + ∑ π΄ππ ππΏπ π΄ π π=1 π π π1 ( π2 ) .. . = ππ π + ∑ ((ππ π) −πΏπ /2 π=1 (5) ππ ) π πΏπ −πΏπ /2 × (ππ π) ((ππ π) ππ π = ππ π + ∑ (πππ (ππ π) are orthonormal. In this case, we take π = ππ π as a solution of the matrix equation (1). −πΏπ /2 ππ ) (12) ) π=1 πΏπ /2 × (ππ π) Proof. If (1) has a solution π, then one can write π as π = ππ π for some nonsingular matrix π. In particular, π can be chosen to be triangular using Theorem 2; thus, we have πΏπ /2 (ππ π) −πΏπ /2 × ((ππ π) π ππ ) π π + ∑ π΄ππ ππΏπ π΄ π = ππ π + ∑ πππ ππ = πΌ. π=1 π=1 π πΏπ = ππ π + ∑ π΄ππ (ππ π) π΄ π (6) π=1 π = ππ π + ∑ π΄ππ (ππ π) πΏπ /2 (ππ π) π=1 πΏπ /2 That is, π is a solution to the matrix equation (1). Theorem 5. The matrix equation (1) has a solution if and only if there exist orthogonal matrices π and π2 and diagonal matrices Γ > 0 and Σ ≥ 0 with ((π + 1)/2)(Γ2 + Σ2 ) = πΌ such that π΄ π. Then (1) can be rewritten as π πΏπ /2 ππ π + ∑ ((ππ π) π=1 π π π=1 (π odd) −πΏπ /2 ∑ π΄ π = ∑ (ππ Γ2 π) π π΄ π ) ((ππ π) πΏπ /2 π΄ π ) = πΌ, (7) ππ+1 Σπ (13) π−1 −πΏπ /2 π 2 + ∑ (π Γ π) or equivalently (π even) π πΏπ /2 [ππ , ∑ ((ππ π) π=1 π [π ] πΏπ /2 π΄ π) ] [ = πΌ. ∑ ((ππ π) π΄ π )] [π=1 ] (8) π In this case, π = ππ Γ2 π is a solution of (1). Proof. Suppose that the matrix equation (1) has a solution. Then from Theorem 4, π΄ π , π = 1, 2, . . . , π, have the form π π π=1 π=1 −πΏπ /2 ∑ π΄ π = ∑ (ππ π) Let π πΏπ /2 ∑ ((ππ π) π=1 π π΄ π ) = ∑ ππ . (9) π=1 Then π π π=1 π=1 ∑ π΄ π = ∑ (ππ π) −πΏπ /2 ππ , (10) ππ+1 Γπ. ππ . (14) Since π π1 ( π2 ) .. . ππ (15) Journal of Applied Mathematics 3 is column-orthonormal, it can be extended to an orthogonal matrix π π π1 π1 ( π2 π2 ) , .. .. . . ππ ππ (16) 0 π1 π π 0 π2 π1 π1 .. ) ( Γ −Σ) (π 0 ) , ( π2 π2 ) = ( ... . Σ Γ 0 π .. .. . . ππ 0 0 ππ+1 ππ ππ (17) where ((π + 1)/2)(Γ2 + Σ2 ) = πΌ. This decomposition is a generalization for Theorem 3 in [15, page 77] and [16, page 37]. It is clear that if we set π = 1, we get the special case of that theorem. Thus π = π1 Γπ, and π π−1 ∑ ππ = ∑ ππ+1 Σπ + ∑ ππ+1 Γπ. π=1 π=1,3 (18) π=2,4 π π π=1 π=1 −πΏπ /2 π = ∑ (ππ Γ2 π) π=1,3 π−1 (19) π π + ∑ π΄ππ ππΏπ π΄ π = (π1 Γπ) (π1 Γπ) −πΏπ /2 + ∑ ((ππ Γ2 π) π=1,3 π 2 −πΏπ /2 π=2,4 −πΏπ /2 π πΏπ ππ+1 Σπ) (ππ Γ2 π) −πΏ2 /2 × ((ππ Γ2 π) −πΏ2 /2 π πΏ2 π3 Γπ) −πΏπ−1 /2 πΏπ−1 π π 2 πΏπ ππ+1 Γπ) (π Γ π) ππ Γπ) ((ππ Γ2 π) π −πΏπ−1 /2 ππ Γπ) −πΏ1 /2 = ππ Γ2 π + (ππ Σπ2π ) (ππ Γ2 π) πΏ1 −πΏ1 /2 × (ππ Γ2 π) (ππ Γ2 π) π2 Σπ −πΏ3 /2 πΏπ −πΏ1 /2 π4 Σπ −πΏπ /2 × (ππ Γ2 π) (ππ Γ2 π) πΏ2 −πΏ2 /2 + (ππ Γπππ ) (ππ Γ2 π) πΏπ−1 −πΏπ /2 ππ+1 Σπ −πΏ2 /2 × (ππ Γ2 π) (ππ Γ2 π) π3 Γπ −πΏπ−1 /2 −πΏπ−1 /2 (ππ Γ2 π) ππ Γπ =ππ Γ2 π+ππ Σπ2π π2 Σπ+ππ Σπ4π π4 Σπ π + ⋅ ⋅ ⋅ +ππ Σππ+1 ππ+1 Σπ =ππ Γ2 π + ππ Σ2 π + ππ Σ2 π + ⋅ ⋅ ⋅ + ππ Σ2 π + ππ Γ2 π + ⋅ ⋅ ⋅ + ππ Γ2 π =ππ ( ππ+1 Γπ) = ππ Γ2 π + ((ππ Γ2 π) ππ+1 Σπ) π3 Γπ) (ππ Γ2 π) + ⋅ ⋅ ⋅ + ((ππ Γ2 π) × (ππ Γ2 π) −πΏπ /2 π +ππ Γπ3π π3 Γπ+ ⋅ ⋅ ⋅ +ππ Γπππ ππ Γπ ππ+1 Σπ) + ∑ ((π Γ π) × ((ππ Γ2 π) + ((ππ Γ2 π) × (ππ Γ2 π) π=1 π−1 ((ππ Γ2 π) + (ππ Γπ3π ) (ππ Γ2 π) ππ+1 Γπ. Conversely, suppose that π΄ π , π = 1, 2, . . . , π have the decomposition (13). Let π = ππ Γ2 π. Then −πΏπ /2 πΏπ ππ+1 Σπ) π + . . . + (ππ Σππ+1 ) (ππ Γ2 π) ππ+1 Σπ π=2,4 × ((ππ Γ2 π) + ⋅ ⋅ ⋅ + ((ππ Γ2 π) × (ππ Γ2 π) πΏ3 π4 Σπ) πΏ3 −πΏπ /2 π −πΏ3 /2 π π4 Σπ) (ππ Γ2 π) × (ππ Γ2 π) (ππ Γ2 π) + ∑ (ππ Γ2 π) π × ((ππ Γ2 π) π2 Σπ) −πΏ3 /2 ππ −πΏπ /2 −πΏ3 /2 −πΏ1 /2 + (ππ Σπ4π ) (ππ Γ2 π) Then (4) can be rewritten as follows: ∑ π΄ π = ∑ (ππ π) + ((ππ Γ2 π) −πΏπ /2 and applying Theorem 3, there exist orthogonal matrices π1 , π2 , . . . , ππ+1 , π, π and diagonal matrices Γ > 0 and Σ ≥ 0 such that π πΏ1 × (ππ Γ2 π) ((ππ Γ2 π) π π2 Σπ) π+1 2 (Γ + Σ2 )) π = ππ π = I. 2 (20) This shows that π is a solution to the matrix equation (1). 4 Journal of Applied Mathematics π π−1 σ΅© σ΅©−πΏπ /2 σ΅© σ΅©−πΏπ /2 = ∑ σ΅©σ΅©σ΅©σ΅©Γ2 σ΅©σ΅©σ΅©σ΅© βΣβ + ∑ σ΅©σ΅©σ΅©σ΅©Γ2 σ΅©σ΅©σ΅©σ΅© βΓβ 4. Main Results π=1,3 In this section, we explain some properties of (1) and we obtain relations between the solution π and the matrices π΄ π . π−1 π=1,3 π=2,4 (22) Since we choose −1 < πΏπ < 0, then we have βΓβ−πΏπ ≤ βΓβ < 1, and therefore π σ΅©σ΅© π σ΅©σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©∑ π΄ π σ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π=1 σ΅©σ΅©σ΅© σ΅©σ΅© π σ΅©σ΅© −πΏπ /2 = σ΅©σ΅©σ΅© ∑ (ππ Γ2 π) ππ+1 Σπ σ΅©σ΅©π=1,3 σ΅© σ΅©σ΅© σ΅©σ΅© −πΏπ /2 ππ+1 Γπσ΅©σ΅©σ΅© + ∑ (ππ Γ2 π) σ΅©σ΅© π=2,4 σ΅© σ΅©σ΅© π σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© −πΏπ /2 ≤ σ΅©σ΅©σ΅© ∑ (ππ Γ2 π) ππ+1 Σπσ΅©σ΅©σ΅© σ΅©σ΅©π=1,3 σ΅©σ΅© σ΅© σ΅© π ≤ ∑ βΓβ−πΏπ βΣβ + ∑ βΓβ−πΏπ βΓβ . Theorem 6. If the matrix equation (1) has a positive definite solution π, then β ∑π π=1 π΄ π β < π. Proof. Suppose that (1) has a solution. Then by Theorem 5, ∑π π=1 π΄ π has the decomposition (13). Then π=2,4 ∑ βΓβ−πΏπ ≤ ( π=1,3 π+1 ), 2 π−1 ∑ βΓβ−πΏπ ≤ ( π=2,4 π−1 ). 2 (23) Thus, σ΅©σ΅© π σ΅©σ΅© σ΅©σ΅© σ΅© σ΅©σ΅©∑ π΄ π σ΅©σ΅©σ΅© ≤ ( π + 1 ) (√ 2 ) σ΅©σ΅© σ΅© 2 π+1 σ΅©σ΅©π=1 σ΅©σ΅©σ΅© π−1 +( (21) σ΅©σ΅© π−1 σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© −πΏπ /2 + σ΅©σ΅©σ΅© ∑ (ππ Γ2 π) ππ+1 Γπσ΅©σ΅©σ΅© σ΅©σ΅©π=2,4 σ΅©σ΅© σ΅© σ΅© π σ΅© −πΏπ /2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©ππ+1 σ΅©σ΅©σ΅©σ΅© βΣβ βπβ ≤ ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) σ΅©σ΅© σ΅© π=1,3 π−1 σ΅© −πΏπ /2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©ππ+1 σ΅©σ΅©σ΅©σ΅© βΓβ βπβ . + ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) σ΅©σ΅© σ΅© π=2,4 2 2 π−1 ) (√ ) = π√ < π. 2 π+1 π+1 (24) The last inequality follows from the fact ((π+1)/2)(Γ2 +Σ2 ) = πΌ, which yields that βΓβ ≤ √2/(π + 1) and βΣβ < √2/(π + 1). In the following theorem, using the necessary and sufficient conditions which we have derived, we state and prove some inequalities in case of the matrix equation (1) having positive definite solution. Theorem 7. Suppose that the matrix equation (1) has a positive definite solution π; then the following hold: −πΏπ π > ∑π (i) ∑π π=1 π π=1 π΄ π π΄ π , Since each ππ+1 , π = 1, 2, . . . , π, is orthogonal, also π is orthogonal. So π πΏπ +1 (πΏπ +1)/2 (ii) πΌ − ∑π π΄ π − ∑π π΄ π π΄ππ π(πΏπ +1)/2 > 0, π=1 π΄ π π π=1 π √ (iii) π(∑π π=1 π΄ π ) ≤ (1/2) 2/(π + 1)((3π − 1)/(π + 1)), σ΅©σ΅© π σ΅©σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©∑ π΄ π σ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π=1 σ΅©σ΅©σ΅© π σ΅© −πΏπ /2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© βΣβ ≤ ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) σ΅©σ΅© π=1,3 σ΅© π−1 σ΅© −πΏπ /2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© βΓβ + ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) σ΅©σ΅© π=2,4 σ΅© π σ΅© σ΅©−πΏπ /2 ≤ ∑ σ΅©σ΅©σ΅©σ΅©ππ Γ2 πσ΅©σ΅©σ΅©σ΅© βΣβ π=1,3 π−1 σ΅© σ΅©−πΏπ /2 + ∑ σ΅©σ΅©σ΅©σ΅©ππ Γ2 πσ΅©σ΅©σ΅©σ΅© βΓβ π=2,4 (1+πΏπ )/2 π (1+πΏπ )/2 (iv) π(∑π π΄ π − ∑π ) ≤ 1, π=1 π π=1 π΄ π π (1+πΏπ )/2 π (1+πΏπ )/2 (v) π(∑π π΄ π + ∑π ) ≤ 1. π=1 π π=1 π΄ π π Proof. (i) By Theorem 4, we have π = ππ π and ∑π π=1 π΄ π = −πΏπ /2 π ∑π π=1 (π π) π π π=1 π=1 ππ . Then ∑ π−πΏπ − ∑ π΄ π π΄ππ π −πΏπ = ∑ (ππ π) π=1 π −πΏπ /2 − ∑ (ππ π) π=1 ππ πππ (ππ π) −πΏπ /2 Journal of Applied Mathematics π = ∑ (ππ π) −πΏπ /2 5 −πΏπ /2 1/2 (ππ π) = (ππ π) π=1 π (πΌ − ∑ ππ πππ ) π=1 π − ∑ (ππ π) −πΏπ /2 π=1 π = ∑ (ππ π) −πΏπ /2 ππ πππ (ππ π) × (ππ π) [πΌ − ∑ ππ πππ ] (ππ π) π=1 −πΏπ /2 (26) > 0, π=1 (25) π = 1, 2, . . . , π, and πΌ−∑π π=1 ππ ππ π π − ∑π=1 ππ ππ > 0. Thus, part (i) since π(ππ πππ ) π π + ∑ πππ (πΌ − ππ π) ππ > 0. π=1 π −πΏπ /2 1/2 π(πππ ππ ), π = π π > 0, and, hence, πΌ proved. π (ii) Replacing πΌ by ππ π + ∑π π=1 ππ ππ , we get This completes the proof of (ii). (iii) Using Theorem 6, we get π π π=1 π=1,3 π (∑ π΄ π ) = π ( ∑ (ππ Γ2 π) = is −πΏπ /2 π−1 ππ+1 Σπ −πΏπ /2 + ∑ (ππ Γ2 π) π=2,4 ππ+1 Γπ) , π π π π=1 π=1 π (∑ π΄ π ) π=1 πΌ − ∑ π΄ππ ππΏπ +1 π΄ π − ∑ π(πΏπ +1)/2 π΄ π π΄ππ π(πΏπ +1)/2 π π π=1 π=1 σ΅¨σ΅¨ π σ΅¨σ΅¨ −πΏπ /2 = max σ΅¨σ΅¨σ΅¨π ( ∑ (ππ Γ2 π) ππ+1 Σπ π σ΅¨σ΅¨ σ΅¨ π=1,3 = ππ π + ∑ πππ ππ − ∑ π΄ππ ππΏπ +1 π΄ π π−1 − ∑ π(πΏπ +1)/2 π΄ π π΄ππ π(πΏπ +1)/2 π=2,4 π π=1 π=1 −πΏπ /2 = ππ π + ∑ πππ ππ − ∑ ((ππ π) πΏπ +1 π × (π π) π − ∑(ππ π) (πΏπ +1)/2 −πΏπ /2 ((ππ π) π=1 × ((ππ π) −πΏπ /2 π ππ ) (ππ π) ππ ) π π −πΏπ /2 ((π π) ππ ) ππ ) (πΏπ +1)/2 π + ∑ (ππ Γ2 π) −πΏπ /2 π−1 σ΅© −πΏπ /2 σ΅© σ΅© σ΅© + ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) Γσ΅©σ΅©σ΅©σ΅© . σ΅© π=2,4 σ΅© π=1 πΏπ +1 × (ππ π) π − ∑(ππ π) (πΏπ +1)/2 −πΏπ /2 (ππ π) −πΏπ /2 ((ππ π) π=1 × (πππ (ππ π) = (ππ π) 1/2 −πΏπ /2 (ππ π) ) (ππ π) 1/2 ππ (27) Since we choose −1 < πΏπ < 0, then we have 0 < (−πΏπ )/2 < ππ ) 1/2 < 1, and therefore (ππ Γ2 π) 1, 2, . . . , π; then (πΏπ +1)/2 π π (∑ π΄ π ) ≤ π π=1 + ∑ πππ ππ 1/2 − ∑ πππ (ππ π) ππ − (ππ π) π=1 π 1/2 ∑ ππ πππ (ππ π) π=1 = −πΏπ /2 ≤ (ππ Γ2 π), π = π + 1 σ΅©σ΅© π 2 σ΅© σ΅©σ΅©(π Γ π) Σσ΅©σ΅©σ΅© σ΅© 2 σ΅© + π=1 π −πΏπ /2 π σ΅© −πΏπ /2 σ΅© σ΅© σ΅© = ∑ σ΅©σ΅©σ΅©σ΅©(ππ Γ2 π) Σσ΅©σ΅©σ΅©σ΅© σ΅© σ΅© π=1,3 π=1 π σ΅©σ΅© σ΅©σ΅© ππ+1 Γπ)σ΅©σ΅©σ΅© σ΅©σ΅© π=2,4 σ΅© σ΅©σ΅© π σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© −πΏπ /2 ≤ σ΅©σ΅©σ΅© ∑ (ππ Γ2 π) ππ+1 Σπσ΅©σ΅©σ΅© σ΅©σ΅©π=1,3 σ΅©σ΅© σ΅© σ΅© σ΅©σ΅© π−1 σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© −πΏπ /2 + σ΅©σ΅©σ΅© ∑ (ππ Γ2 π) ππ+1 Γπσ΅©σ΅©σ΅© σ΅©σ΅©π=2,4 σ΅©σ΅© σ΅© σ΅© π−1 = ππ π + ∑ πππ ππ − ∑ πππ (ππ π) σ΅¨σ΅¨ σ΅¨σ΅¨ ππ+1 Γπ)σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅©σ΅© π σ΅©σ΅© −πΏπ /2 ≤ σ΅©σ΅©σ΅©( ∑ (ππ Γ2 π) ππ+1 Σπ σ΅©σ΅© π=1,3 σ΅© π=1 π −πΏπ /2 + ∑ (ππ Γ2 π) π π − 1 σ΅©σ΅© π 2 σ΅© σ΅©σ΅©(π Γ π) Γσ΅©σ΅©σ΅© σ΅© 2 σ΅© π + 1 σ΅©σ΅© π 2 σ΅©σ΅© π − 1 σ΅©σ΅© π 3 σ΅©σ΅© σ΅©σ΅©π ΣΓ πσ΅©σ΅© + σ΅©σ΅©π Γ πσ΅©σ΅© σ΅© σ΅© 2 σ΅© 2 σ΅© 6 Journal of Applied Mathematics = ≤ ≤ π + 1 σ΅©σ΅© 2 σ΅©σ΅© π − 1 σ΅©σ΅© 3 σ΅©σ΅© σ΅©σ΅©ΣΓ σ΅©σ΅© + σ΅©σ΅©Γ σ΅©σ΅© 2 σ΅© σ΅© 2 σ΅© σ΅© π ± (∑ (ππ π) π=1 π+1 π−1 3 βΣΓΓβ + βΓβ 2 2 π 1/2 ππ + ∑ πππ (ππ π) ) π=1 1/2 = ((ππ π) π−1 3 π+1 βΣΓβ βΓβ + βΓβ . 2 2 1/2 π π ± ∑ ππ ) ((ππ π) π=1 1/2 π ± ∑ ππ ) ≥ 0. π=1 (31) (28) Let Σ = diag(ππ ), Γ = diag(πΎπ ). Then ((π + 1)/2)(ππ2 + πΎπ2 ) = 1. Thus π (∑ π΄ π ) π=1 3 π−1 2 2 π+1 √ (√ ) βΣΓβ + 2 π+1 2 π+1 = 2 2 π+1 π−1 √ max {ππ πΎπ } + (√ ) 2 π+1 π 2 π+1 3 References 3 ππ2 + πΎπ2 π − 1 2 2 π+1 √ √ ≤ max + ( ) 2 π+1 π 2 2 π+1 2 1 3π − 1 = √ ( ). 2 π+1 π+1 (29) (iv) Appling Lemma 1, we get π π π=1 π=1 π (∑ π(1+πΏπ )/2 π΄ π − ∑ π΄ππ π(1+πΏπ )/2 ) π = π (∑ (ππ π) (1+πΏπ )/2 −πΏπ /2 (ππ π) π=1 π − ∑ πππ (ππ π) −πΏπ /2 ππ (1+πΏπ )/2 (ππ π) ) π=1 π = π (∑ (ππ π) 1/2 π=1 π ππ − ∑ πππ (ππ π) π=1 π ≤ π ((ππ π) + ∑ πππ ππ ) = π (πΌ) = 1. π=1 (v) Consider π π π=1 π=1 πΌ ± (∑ π(1+πΏπ )/2 π΄ π + ∑ π΄ππ π(1+πΏπ )/2 ) π = ππ π + ∑ πππ ππ π=1 1/2 ) 5. Conclusion In this paper, both necessary and sufficient conditions for π πΏπ the nonlinear matrix equation π + ∑π π=1 π΄ π π π΄ π = πΌ to have a positive definite solution π are given, where −1 < πΏπ < 0, π΄ π are π × π nonsingular real matrices, and π is an odd positive integer. Some properties of this matrix equation are explained. 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