Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 781983, 6 pages http://dx.doi.org/10.1155/2013/781983 Research Article ℎ-Stability of Linear Matrix Differential Systems Peiguang Wang1 and Xiaowei Liu2 1 2 College of Electronic and Information Engineering, Hebei University, Baoding, Hebei 071002, China College of Mathematics and Computer Science, Hebei University, Baoding, Hebei 071002, China Correspondence should be addressed to Peiguang Wang; pgwang@mail.hbu.edu.cn Received 2 December 2012; Accepted 1 February 2013 Academic Editor: Yong Hong Wu Copyright © 2013 P. Wang and X. Liu. 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. This paper investigates the stability problem of linear matrix differential systems and gives some sufficient conditions of ℎ-stability for linear matrix system and its associated perturbed system by using the Kronecker product of matrices. An example is also worked out to illustrate our results. 1. Introduction The theory of stability in the sense of Lyapunov is well known and is used in the real world. It is obvious that, in applications, asymptotic stability is more important than stability because the desirable feature is to know the size of the region of asymptotic stability. However, when we study the asymptotic stability, it is not easy to work with nonexponential types of stability. In recent years, Medina and Pinto [1, 2] extended the study of exponential stability to a variety of reasonable systems called ℎ-systems. They introduced the notion of ℎstability with the intention of obtaining results about stability for a weakly stable system (at least, weaker than those given exponential stability and the uniform Lipschitz stability) under some perturbations. Choi et al. [3] investigated ℎstability for the nonlinear differential systems by employing the notion of 𝑡∞ -similarity and the Lyapunov functions. And then, Choi et al. [4–6] also characterized the ℎ-stability in variation for nonlinear difference systems via 𝑛∞ -similarity and the Lyapunov functions and obtained some results related to stability for the perturbations of nonlinear difference systems. However, as far as the author’s scope, there are few discussions and results for matrix differential systems. In this paper, we shall investigate the ℎ-stability problem for linear matrix differential systems by employing the Kronecker product of matrices which can be found in Lakshmikantham and Deo’s monograph [7]. Some preliminaries are presented in Section 2. A theorem is given in this section, which is important to complete the main results of this paper. In Section 3, sufficient conditions for the ℎ-stability are given for linear matrix system and its associated perturbed system. An example is also worked out at the end of this paper. 2. Preliminaries Consider the linear matrix differential equation 𝑋 = 𝐴 (𝑡) 𝑋 + 𝑋𝐵 (𝑡) , 𝑋 (𝑡0 ) = 𝑋0 (1) and its associated perturbed system 𝑌 = 𝐴 (𝑡) 𝑌 + 𝑌𝐵 (𝑡) + 𝑅 (𝑡, 𝑌) , 𝑌 (𝑡0 ) = 𝑋0 , (2) where 𝐴, 𝐵 ∈ 𝐶[𝑅+ , 𝑅𝑛×𝑛 ], 𝑅 ∈ 𝐶[𝑅+ ×𝑅𝑛×𝑛 , 𝑅𝑛×𝑛 ], 𝑅(𝑡, 0) ≡ 0, and 𝑋, 𝑌 ∈ 𝑅𝑛×𝑛 . Now, we introduce the vec (⋅) operator which maps an 𝑚 × 𝑛 matrix 𝑃 = (𝑝𝑖𝑗 ) onto the vector composed of the rows of 𝑃 𝑇 vec (𝑃) = (𝑝11 , . . . , 𝑝1𝑛 , 𝑝21 , . . . , 𝑝2𝑛 , . . . , 𝑝𝑚1 , . . . , 𝑝𝑚𝑛 ) . (3) Let us begin by defining the Kronecker product of matrices. 2 Abstract and Applied Analysis Definition 1 (see [7]). If 𝑃 ∈ 𝑅𝑐×𝑑 , 𝑄 ∈ 𝑅𝑚×𝑛 , then the Kronecker product of 𝑃 and 𝑄, 𝑃 ⊗ 𝑄 ∈ 𝑅𝑐𝑚×𝑑𝑛 , is defined by the matrix Lemma 3 (see [7]). Assume that 𝑥(𝑡, 𝑡0 , 𝑥0 ) is the solution of (7) through (𝑡0 , 𝑥0 ), which exists for 𝑡 ≥ 𝑡0 , then 𝑝11 𝑄 𝑝12 𝑄 ⋅ ⋅ ⋅ 𝑝1𝑑 𝑄 𝑝21 𝑄 𝑝22 𝑄 ⋅ ⋅ ⋅ 𝑝2𝑑 𝑄 . . . . ) ( 𝑃⊗𝑄= . . . . . 𝑝𝑐1 𝑄 𝑝𝑐2 𝑄 ⋅ ⋅ ⋅ 𝑝𝑐𝑑 𝑄 𝑥 (𝑡, 𝑡0 , 𝑥0 ) = [∫ Φ (𝑡, 𝑡0 , 𝑠𝑥0 ) 𝑑𝑠]𝑥0 , ( 0 (4) Among the main properties of this product presented in [8], we recall the following useful ones: (1) vec (𝑃𝑋𝑄) = (𝑃 ⊗ 𝑄𝑇 )vec (𝑋), (2) vec (𝑃𝑋 + 𝑋𝑄) = (𝑃 ⊗ 𝐼 + 𝐼 ⊗ 𝑄𝑇 )vec (𝑋), 𝑦 = (𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 ) 𝑦 + 𝑟 (𝑡, 𝑦) , where Φ(𝑡, 𝑡0 , 𝑥0 ) = 𝜕𝑥(𝑡, 𝑡0 , 𝑥0 )/𝜕𝑥0 . Theorem 4. Assume that 𝑥(𝑡, 𝑡0 , 𝑥0 ) is the solution of (5) for 𝑡 ≥ 𝑡0 , let 𝐺 (𝑡, 𝑡0 , 𝑥0 ) = 𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 . where 𝑃, 𝑋, 𝑄, and 𝐼 ∈ 𝑅𝑛×𝑛 and 𝐼 is an identity matrix. Then, the equivalent vector differential systems of (1) and (2) can be written as 𝑥 (𝑡0 ) = 𝑥0 , 𝜑 = 𝐺 (𝑡, 𝑡0 , 𝑥0 ) 𝜑, (5) 2 where 𝑥 = vec (𝑋), 𝑦 = vec (𝑌), 𝑟 = vec (𝑅), 𝑟 ∈ 𝐶(𝑅+ × 𝑅𝑛 , 2 𝑅𝑛 ), and 𝑟(𝑡, 0) ≡ 0. In order to investigate ℎ-stability of linear matrix equation and its associated perturbed system, we need to consider the following systems and their properties. The techniques and results are similar to those of [7]. Consider the linear differential system (7) where 𝑃 is an 𝑛 × 𝑛 continuous matrix and its perturbation 𝑦 = 𝑃 (𝑡)𝑦 + 𝐹 (𝑡, 𝑦) , + 𝑛 𝑦 (𝑡0 ) = 𝑥0 , Φ (𝑡, 𝑡0 , 𝑥0 ) = 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 ) , 𝑊 = 𝐴 (𝑡) 𝑊, 𝑊 (𝑡0 ) = 𝐼, (15) 𝑍 = 𝑍𝐵 (𝑡) , 𝑍 (𝑡0 ) = 𝐼, (16) respectively. (ii) Any solution of (2) satisfies the integral equation 𝑌 (𝑡, 𝑡0 , 𝑋0 ) = 𝑋 (𝑡, 𝑡0 , 𝑋0 ) 𝑡 + ∫ 𝑊 (𝑡, 𝑠) 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑋0 )) 𝑍 (𝑡, 𝑠) 𝑑𝑠, (8) where 𝐹 ∈ 𝐶[𝑅 × 𝑅 , 𝑅 ]. Suppose that the solution 𝑥(𝑡, 𝑡0 , 𝑥0 ) of (7) exists for all 𝑡 ≥ 𝑡0 . The fundamental matrix solution Φ(𝑡, 𝑡0 , 𝑥0 ) of (7) is given by [7] (9) and Φ(𝑡0 , 𝑡0 , 𝑥0 ) = 𝐼. We are now in a position to give the Alekseev formula, which connects the solutions of (7) and (8). Lemma 2 (see [7]). If 𝑥(𝑡, 𝑡0 , 𝑥0 ) is the solution of (7) and exists for 𝑡 ≥ 𝑡0 , any solution 𝑦(𝑡, 𝑡0 , 𝑥0 ) of (8), with 𝑦(𝑡0 ) = 𝑥0 , satisfies the integral equation 𝑡0 (17) for 𝑡 ≥ 𝑡0 . Proof. (i) It is obvious that Φ(𝑡, 𝑡0 , 𝑥0 ) = 𝜕𝑥(𝑡, 𝑡0 , 𝑥0 )/𝜕𝑥0 exists and is the fundamental matrix solution of the variational equation 𝜑 = 𝐺 (𝑡, 𝑡0 , 𝑥0 ) 𝜑, (18) such that Φ(𝑡0 , 𝑡0 , 𝑥0 ) = 𝐼. Furthermore, we get 𝜑 = 𝐺 (𝑡, 𝑡0 , 𝑥0 ) 𝜑 = [𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 ] 𝜑, (19) with the initial value 𝑦 (𝑡, 𝑡0 , 𝑥0 ) = 𝑥 (𝑡, 𝑡0 , 𝑥0 ) 𝑡 + ∫ Φ (𝑡, 𝑠, 𝑦 (𝑠, 𝑡0 , 𝑥0 )) 𝐹 (𝑠, 𝑦 (𝑠, 𝑡0 , 𝑥0 ))𝑑𝑠, 𝑡0 (10) for 𝑡 ≥ 𝑡0 , where Φ(𝑡, 𝑡0 , 𝑥0 ) = 𝜕𝑥(𝑡, 𝑡0 , 𝑥0 )/𝜕𝑥0 . (14) where 𝑊(𝑡, 𝑡0 ) and 𝑍(𝑡, 𝑡0 ) are solutions of 𝑛 𝜕𝑥 (𝑡, 𝑡0 , 𝑥0 ) Φ (𝑡, 𝑡0 , 𝑥0 ) = 𝜕𝑥0 (13) such that Φ(𝑡0 , 𝑡0 , 𝑥0 ) = 𝐼, and therefore 𝑦 (𝑡0 ) = 𝑥0 , 𝑥 (𝑡0 ) = 𝑥0 , (12) Then one has the following. (i) Φ(𝑡, 𝑡0 , 𝑥0 ) = 𝜕𝑥(𝑡, 𝑡0 , 𝑥0 )/𝜕𝑥0 exists and is the fundamental matrix solution of the variational equation (6) 𝑥 = 𝑃 (𝑡) 𝑥, (11) The following theorem gives an analog of the variation of parameters formula for the solution of (2). ) 𝑥 = (𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 ) 𝑥, 1 𝜑 (𝑡0 , 𝑡0 , 𝑥0 ) = 𝑒, 𝑒 = vec (𝐼) , (20) which has the solution 𝜑 (𝑡, 𝑡0 , 𝑥0 ) = (𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 )) 𝑒, (21) Abstract and Applied Analysis 3 where 𝑊 and 𝑍 are the solutions of (15) and (16), respectively, and 𝐼 is the 𝑛 × 𝑛 identity matrix. Therefore, Φ (𝑡, 𝑡0 , 𝑥0 ) = 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 ) . (22) (ii) Employing Lemma 2 and substituting for Φ the righthand side of (22), we get 𝑦 (𝑡, 𝑡0 , 𝑥0 ) = 𝑥 (𝑡, 𝑡0 , 𝑥0 ) 𝑡 + ∫ [𝑊 (𝑡, 𝑠) ⊗ 𝑍𝑇 (𝑡, 𝑠)] 𝑟 (𝑠, 𝑦 (𝑠, 𝑡0 , 𝑥0 ))𝑑𝑠 𝑡0 (23) for 𝑡 ≥ 𝑡0 , where 𝑦(𝑡, 𝑡0 , 𝑥0 ) is any solution of (6). Now, we define 𝑋(𝑡, 𝑡0 , 𝑋0 ), 𝑌(𝑡, 𝑡0 , 𝑋0 ), and 𝑅(𝑡, 𝑌) by 𝑥 = vec (𝑋), 𝑦 = vec (𝑌), and 𝑟 = vec (𝑅). Thus, we have that Lemma 7 (see [4]). The linear system 𝑥 = 𝐴 (𝑡) 𝑥, 𝑥 (𝑡0 ) = 𝑥0 , is ℎ𝑆 if and only if there exist a constant 𝑐 ≥ 1 and a positive continuous bounded function ℎ defined on 𝑅+ such that for every 𝑥0 in 𝑅𝑛 , −1 Φ (𝑡, 𝑡0 , 𝑥0 ) ≤ 𝑐ℎ (𝑡) ℎ (𝑡0 ) Theorem 8. The solution 𝑋 = 0 of (1) is ℎ𝑆 if and only if the solution 𝑥 = 0 of (5) is ℎ𝑆. Proof. Necessity. Since the solution 𝑋 = 0 of (1) is ℎ𝑆, there exist 𝑐 ≥ 1, 𝛿 > 0, and a positive bounded continuous function ℎ on 𝑅+ such that −1 𝑋 (𝑡, 𝑡0 , 𝑋0 ) ≤ 𝑐 𝑋0 ℎ (𝑡) ℎ (𝑡0 ) + ∫ 𝑊 (𝑡, 𝑠) 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑋0 )) 𝑍 (𝑡, 𝑠) 𝑑𝑠, 𝑡0 (24) for 𝑡 ≥ 𝑡0 , where 𝑋(𝑡, 𝑡0 , 𝑋0 ) is the unique solution of (1) for 𝑡 ≥ 𝑡0 . The proof is completed. 𝑋 = 𝐴 (𝑡) 𝑋 + 𝑋𝐵 (𝑡) , 𝑋 (𝑡0 ) = 𝑋0 , (31) It follows that 𝑚×𝑛 Definition 5. A generalized matrix valued norm from 𝑅 𝑅+ is a mapping ‖ ⋅ ‖ : 𝑅𝑚×𝑛 → 𝑅+ such that [vec (𝑋)] = (𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 ) vec (𝑋) , to (32) Thus, 𝑥 (𝑡, 𝑡0 , 𝑥0 ) = vec (𝑋 (𝑡, 𝑡0 , 𝑋0 )) = 𝑋 (𝑡, 𝑡0 , 𝑋0 ) ≤ 𝑐 𝑥0 ℎ (𝑡) ℎ−1 (𝑡0 ) . (a) ‖𝑋‖ ≥ 0, ‖𝑋‖ = 0 if and only if 𝑋 = 0, (b) ‖𝜆𝑋‖ = |𝜆|‖𝑋‖, 𝜆 is a constant, (c) ‖𝑋 + 𝑌‖ ≤ ‖𝑋‖ + ‖𝑌‖. Definition 6. The zero solution of (1) is said to be (hS) ℎ-stability if there exist 𝑐 ≥ 1, 𝛿 > 0, and a positive bounded continuous function ℎ on 𝑅+ such that (25) for 𝑡 ≥ 𝑡0 ≥ 0 and ‖𝑋0 ‖ ≤ 𝛿, ℎ−1 (𝑡0 ) = 1/ℎ(𝑡0 ). (hSV) ℎ-stability in variation if there exist 𝑐1 , 𝑐2 ≥ 1, 𝛿 > 0, and a positive bounded continuous function ℎ on 𝑅+ satisfying −1 𝑊 (𝑡, 𝑡0 ) ≤ 𝑐1 ℎ (𝑡) ℎ (𝑡0 ) , 𝑍 (𝑡, 𝑡0 ) ≤ 𝑐2 ℎ (𝑡) ℎ−1 (𝑡0 ) , (30) then we obtain We firstly give some notions. −1 𝑋 (𝑡, 𝑡0 , 𝑋0 ) ≤ 𝑐 𝑋0 ℎ (𝑡) ℎ (𝑡0 ) , (29) for every 𝑡 ≥ 𝑡0 ≥ 0, ‖𝑋0 ‖ ≤ 𝛿, where 𝑋(𝑡, 𝑡0 , 𝑋0 ) is the solution of (1), satisfying vec (𝑋 ) = vec (𝐴 (𝑡) 𝑋 + 𝑋𝐵 (𝑡)) . 3. Main Results (28) for all 𝑡 ≥ 𝑡0 ≥ 0, where 𝐴(𝑡) is an 𝑛 × 𝑛 continuous matrix and Φ(𝑡, 𝑡0 , 𝑥0 ) is a fundamental matrix of (27). 𝑌 (𝑡, 𝑡0 , 𝑋0 ) = 𝑋 (𝑡, 𝑡0 , 𝑋0 ) 𝑡 (27) (26) provided ‖𝑋0 ‖ ≤ 𝛿, where 𝑊(𝑡, 𝑡0 ) and 𝑍(𝑡, 𝑡0 ) are given in Theorem 4. (33) Sufficiency. It can be easily proved by the same method. The proof is completed. Theorem 9. The solution 𝑋 = 0 of (1) is ℎ𝑆 if and only if there exist a constant 𝑐 ≥ 1 and a positive continuous bounded function ℎ defined on 𝑅+ such that for every 𝑋0 in 𝑅𝑛×𝑛 , 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 ) ≤ 𝑐ℎ (𝑡) ℎ−1 (𝑡0 ) (34) for all 𝑡 ≥ 𝑡0 ≥ 0. Proof. Sufficiency. Following Lemma 3 and Theorem 4, we have 1 𝑥 (𝑡, 𝑡0 , 𝑥0 ) = [∫ Φ (𝑡, 𝑡0 , 𝑠𝑥0 )𝑑𝑠] 𝑥0 , 0 𝑇 Φ (𝑡, 𝑡0 , 𝑥0 ) = 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍 (𝑡, 𝑡0 ) . (35) 4 Abstract and Applied Analysis 2 (ii) ‖𝑥‖ ≤ 𝑉(𝑡, 𝑥) ≤ 𝑐‖𝑥‖, (𝑡, 𝑥) ∈ 𝑅+ × 𝑅𝑛 , 𝑐 ≥ 1, It follows that 2 1 𝑇 𝑥 (𝑡, 𝑡0 , 𝑥0 ) = [∫ 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍 (𝑡, 𝑡0 )𝑑𝑠]𝑥0 . 0 (36) Hence, 1 𝑇 𝑥 (𝑡, 𝑡0 , 𝑥0 ) ≤ 𝑥0 ∫ 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍 (𝑡, 𝑡0 ) 𝑑𝑠 0 ≤ 𝑐 𝑥0 ℎ (𝑡) ℎ−1 (𝑡0 ) , 𝑡 ≥ 𝑡0 . (iii) 𝐷+ 𝑉(5) (𝑡, 𝑥) ≤ ℎ (𝑡)ℎ−1 (𝑡)𝑉(𝑡, 𝑥), (𝑡, 𝑥) ∈ 𝑅+ × 𝑅𝑛 . Then, the solution 𝑋 = 0 of (1) is ℎ𝑆. Proof. Let 𝑥(𝑡, 𝑡0 , 𝑥0 ) be the solution of (5). As a consequence of (iii), we obtain (37) 𝑉 (𝑡, 𝑋 (𝑡, 𝑡0 , 𝑥0 )) ≤ 𝑉 (𝑡0 , 𝑥0 ) exp ∫ 𝑡0 Therefore, the solution 𝑥 = 0 of (5) is ℎ𝑆. By Theorem 8, it implies that the solution 𝑋 = 0 of (1) is ℎ𝑆. Necessity. If the solution 𝑋 = 0 of (1) is ℎ𝑆, then the solution 𝑥 = 0 of (5) is ℎ𝑆 using Theorem 8. By Lemma 7, we have −1 (38) Φ (𝑡, 𝑡0 , 𝑥0 ) ≤ 𝑐ℎ (𝑡) ℎ (𝑡0 ) . From Theorem 4, we obtain that Φ (𝑡, 𝑡0 , 𝑥0 ) = 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 ) , = 𝑉 (𝑡0 , 𝑥0 ) ℎ (𝑡) ℎ (𝑡0 ) . From the condition (ii), we have −1 𝑥 (𝑡, 𝑡0 , 𝑥0 ) ≤ 𝑐 𝑥0 ℎ (𝑡) ℎ (𝑡0 ) , By Theorem 8, we can easily get that the solution 𝑋 = 0 of (1) is ℎ𝑆. The proof is completed. 𝑡 𝑡 𝑡0 𝑡0 𝑥 (𝑡) − ∫ 𝑘 (𝑠, 𝑥 (𝑡))𝑑𝑠 ≤ 𝑦 (𝑡) − ∫ 𝑘 (𝑠, 𝑦 (𝑡)) 𝑑𝑠, 1 𝛿 (46) 𝑡 ≥ 𝑡0 ≥ 0 for 𝑥, 𝑦 ∈ 𝐶([𝑡0 , ∞), 𝑅𝑛 ). If 𝑥(𝑡0 ) < 𝑦(𝑡0 ), then 𝑥(𝑡) < 𝑦(𝑡) for all 𝑡 ≥ 𝑡0 ≥ 0. Theorem 13. Assume that 𝑋 = 0 of (1) is ℎ𝑆𝑉 with the nonincreasing function ℎ1 and ℎ2 . Consider the scalar differential equation 𝑢 = 𝑐𝑙 (𝑡, 𝑢) , × [𝑉 (𝑡 + 𝛿, 𝑥 + 𝛿 (𝐴 ⊗ 𝐼 + 𝐼 ⊗ 𝐵𝑇 ) 𝑥) 𝑢 (𝑡0 ) = 𝑢0 , 𝑤ℎ𝑒𝑟𝑒 𝑐 ≥ 1. (47) Suppose that ‖𝑅 (𝑡, 𝑌)‖ ≤ 𝑙 (𝑡, ‖𝑌‖) , −𝑉 (𝑡, 𝑥) ] , (41) 2 for (𝑡, 𝑥) ∈ 𝑅+ × 𝑅𝑛 and for the solution 𝑥(𝑡) = 𝑥(𝑡, 𝑡0 , 𝑥0 ) of (5), 𝛿→0 (45) (40) Next, we offer sufficient conditions for the ℎ-stability of linear matrix differential systems by using the Lyapunov functions. Defining the Lyapunov functions 𝐷+ 𝑉 (𝑡, 𝑥) = lim sup 𝑡 ≥ 𝑡0 ≥ 0. Lemma 12 (see [9]). Suppose that 𝑘(𝑡, 𝑥) ∈ 𝐶(𝑅+ × 𝑅𝑛 , 𝑅𝑛 ) is strictly increasing in 𝑥 for 𝑡 ≥ 𝑡0 ≥ 0 with the property Corollary 10. If the zero solution of (1) is ℎ𝑆𝑉, then the zero solution of (1) is ℎ𝑆. 𝛿→0 (44) −1 Now, we examine the properties of the perturbed linear matrix differential system. This completes the proof. 𝐷+ 𝑉(5) (𝑡, 𝑥) = lim sup ℎ (𝑠) 𝑑𝑠 ℎ (𝑠) (39) Thus, 𝑊 (𝑡, 𝑡0 ) ⊗ 𝑍𝑇 (𝑡, 𝑡0 ) ≤ 𝑐ℎ (𝑡) ℎ−1 (𝑡0 ) . 𝑡 1 [𝑉 (𝑡 + 𝛿, 𝑥 (𝑡 + 𝛿)) − 𝑉 (𝑡, 𝑥)] . 𝛿 (42) (48) where 𝑙 ∈ 𝐶(𝑅+ × 𝑅+ , 𝑅+ ) is strictly increasing in 𝑢 for each fixed 𝑡 ≥ 𝑡0 ≥ 0 with 𝑙(𝑡, 0) = 0. If 𝑢 = 0 is ℎ𝑆, then the solution 𝑌 = 0 of (2) is also ℎ𝑆, whenever 𝑢0 = 𝑐‖𝑌0 ‖. Proof. By Theorem 4, the solutions of (1) and (2) with the same initial values are related by 𝑌 (𝑡, 𝑡0 , 𝑌0 ) = 𝑋 (𝑡, 𝑡0 , 𝑌0 ) Then, it is well known that 𝑡 𝐷+ 𝑉(5) (𝑡, 𝑥) = 𝐷+ 𝑉 (𝑡, 𝑥) , + ∫ 𝑊 (𝑡, 𝑠) 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑌0 )) 𝑍 (𝑡, 𝑠)𝑑𝑠. (43) 𝑡0 + (49) if 𝑉(𝑡, 𝑥) is the Lipschitzian in 𝑥 for each 𝑡 ∈ 𝑅 . Theorem 11. Suppose that ℎ(𝑡) is a positive bonded continuously differentiable function on 𝑅+ . Furthermore, assume that there exists a function 𝑉(𝑡, 𝑥) satisfying the following properties: 2 (i) 𝑉 ∈ 𝐶(𝑅+ × 𝑅𝑛 , 𝑅+ ), and 𝑉(𝑡, 𝑥) is Lipschitzian in 𝑥 for each 𝑡 ∈ 𝑅+ , Then, we have 𝑡 𝑌 (𝑡, 𝑡0 , 𝑌0 ) ≤ 𝑋 (𝑡, 𝑡0 , 𝑌0 ) + ∫ ‖𝑊 (𝑡, 𝑠)‖ 𝑡 0 × 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑌0 )) ‖Z (𝑡, 𝑠)‖ 𝑑𝑠. (50) Abstract and Applied Analysis 5 From Corollary 10, it easily follows that −1 𝑌 (𝑡, 𝑡0 , 𝑌0 ) ≤ 𝑐1 𝑌0 ℎ1 (𝑡) ℎ1 (𝑡0 ) 𝑡 + ∫ 𝑐2 𝑐3 [ℎ2 (𝑡) ℎ2−1 (𝑠)] Then, by Gronwall’s inequality, we get −1 𝑌 (𝑡, 𝑡0 , 𝑋0 ) ≤ 𝑐 𝑋0 ℎ (𝑡) ℎ (𝑡0 ) ∞ 2 𝑡0 × 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑌0 ))𝑑𝑠 2 × exp (∫ 𝑐1 𝑐2 [ℎ1 (𝑡) ℎ1−1 (𝑠)] 𝛾 (𝑠) 𝑑𝑠) 𝑡0 (51) ≤ 𝑀 𝑋0 ℎ (𝑡) ℎ−1 (𝑡0 ) , (56) 𝑡 ≤ 𝑐 𝑌0 + 𝑐 ∫ 𝑙 (𝑠, ‖𝑌 (𝑠)‖) 𝑑𝑠, 𝑡 ∞ 0 where 𝑐 = max{𝑐1 , 𝑐2 𝑐3 }. Since ℎ1 (𝑡) and ℎ2 (𝑡) are nonincreasing, we obtain 4. Example 𝑡 𝑌 (𝑡, 𝑡0 , 𝑌0 ) − 𝑐 ∫ 𝑙 (𝑠, ‖𝑌 (𝑠)‖)𝑑𝑠 𝑡0 𝑡 ≤ 𝑐 𝑌0 = 𝑢0 = 𝑢 (𝑡) − ∫ 𝑐𝑙 (𝑠, 𝑢 (𝑠))𝑑𝑠. (52) 𝑡0 By Lemma 12, we have ‖𝑌(𝑡)‖ < 𝑢(𝑡) for all 𝑡 ≥ 𝑡0 ≥ 0. Since 𝑢 = 0 of (47) is ℎ𝑆, In this section, we give a simple but illustrative example. Consider the matrix differential equation −1 1 −1 0 𝑋 (𝑡) = ( ) 𝑋 (𝑡) + 𝑋 (𝑡) ( ), 0 −2 0 −1 1 0 𝑋 (0) = ( ). 0 1 ‖𝑌 (𝑡)‖ < 𝑢 (𝑡) ≤ 𝑐4 𝑢0 ℎ (𝑡) ℎ−1 (𝑡0 ) = 𝑐4 𝑐 𝑌0 ℎ (𝑡) ℎ−1 (𝑡0 ) = 𝑀 𝑌0 ℎ (𝑡) ℎ−1 (𝑡0 ) , 2 where 𝑀 = max{𝑐 exp(∫𝑡 𝑐1 𝑐2 [ℎ1 (𝑡)ℎ1−1 (𝑠)] 𝛾(𝑠)𝑑𝑠)}. 0 The proof is completed. Then, we can obtain the following equations: Theorem 14. Assume that −1 1 ) 𝑊, 0 −2 𝑊 (0) = 𝐼, (58) −1 0 ), 𝑍 = 𝑍 ( 0 −1 𝑍 (0) = 𝐼. (59) 𝑊 = ( 𝑐4 ≥ 1, 𝑀 = 𝑐4 𝑐 ≥ 1. (53) This completes the proof. The solutions of (58) and (59) are (i) the zero solution of (1) is ℎ𝑆𝑉, (ii) ‖𝑅(𝑡, 𝑌(𝑡))‖ ≤ 𝛾(𝑡)‖𝑌(𝑡)‖ provided that 𝛾(𝑡) > 0 and ∞ ∫𝑡 𝛾(𝑡)𝑑𝑡 < ∞ for 𝑡0 ≥ 0. 𝑒−𝑡 𝑒−𝑡 − 𝑒−2𝑡 ), 𝑊 (𝑡) = ( 0 𝑒−2𝑡 𝑍 (𝑡) = ( 𝑒−𝑡 0 ), 0 𝑒−𝑡 (60) 0 Then, the solution 𝑌 = 0 of (2) is ℎ𝑆. Proof. By Theorem 4, the solutions of (1) and (2) with the same initial values are related by 𝑌 (𝑡, 𝑡0 , 𝑋0 ) = 𝑋 (𝑡, 𝑡0 , 𝑋0 ) 𝑡 + ∫ 𝑊 (𝑡, 𝑠) 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑋0 )) 𝑍 (𝑡, 𝑠)𝑑𝑠. 𝑡0 (54) 𝑒−2𝑡 0 𝑒−2𝑡 − 𝑒−3𝑡 0 −2𝑡 −2𝑡 0 𝑒 − 𝑒−3𝑡 0 𝑒 ). 𝑊 (𝑡) ⊗ 𝑍𝑇 (𝑡) = ( −3𝑡 0 0 𝑒 0 −3𝑡 0 0 0 𝑒 (61) Thus, we have 𝑡 𝑡0 × ‖𝑍 (𝑡, 𝑠)‖ 𝑑𝑠 ≤ 𝑐 𝑋0 ℎ (𝑡) ℎ−1 (𝑡0 ) Acknowledgments 2 𝑡0 × 𝛾 (𝑠) 𝑌 (𝑠, 𝑡0 , 𝑋0 ) 𝑑𝑠. (62) where ℎ(𝑡) = 𝑒−2𝑡 , 𝑐 = 5, ‖𝑊(𝑡) ⊗ 𝑍𝑇 (𝑡)‖ = 4𝑒−2𝑡 , ‖𝐷‖ = 𝑚×𝑛 , and 𝐼 is an identity matrix. So, from ∑𝑚,𝑛 𝑖,𝑗 |𝑑𝑖𝑗 |, 𝐷 ∈ 𝑅 Theorem 9, we can conclude that the solution 𝑋 = 0 of (57) is ℎ𝑆. + ∫ ‖𝑊 (𝑡, 𝑠)‖ 𝑅 (𝑠, 𝑌 (𝑠, 𝑡0 , 𝑋0 )) + ∫ 𝑐1 𝑐2 [ℎ1 (𝑡) ℎ1−1 (𝑠)] respectively. Then, 𝑊 (𝑡) ⊗ 𝑍𝑇 (𝑡) ≤ 𝑐ℎ (𝑡) ℎ−1 (0) , The assumptions (i) and (ii) yield 𝑌 (𝑡, 𝑡0 , 𝑋0 ) ≤ 𝑋 (𝑡, 𝑡0 , 𝑋0 ) 𝑡 (57) (55) The authors would like to thank the reviewers for their valuable suggestions and comments. This paper is supported by the National Natural Science Foundation of China (10971045 and 11271106). 6 References [1] R. Medina and M. Pinto, “Variationally stable difference equations,” Nonlinear Analysis, vol. 30, no. 2, pp. 1141–1152, 1997. [2] M. Pinto, “Perturbations of asymptotically stable differential systems,” Analysis, vol. 4, no. 1-2, pp. 161–175, 1984. [3] S. K. Choi, N. J. Koo, and H. S. Ryu, “h-stability of differential systems via 𝑡∞ -similarity,” Bulletin of the Korean Mathematical Society, vol. 34, no. 3, pp. 371–383, 1997. [4] S. K. Choi and N. J. Koo, “Variationally stable difference systems by 𝑛∞ -similarity,” Journal of Mathematical Analysis and Applications, vol. 249, no. 2, pp. 553–568, 2000. [5] S. K. Choi, N. J. Koo, and Y. H. Goo, “Variationally stable difference systems,” Journal of Mathematical Analysis and Applications, vol. 256, no. 2, pp. 587–605, 2001. [6] S. K. Choi, N. J. Koo, and S. M. Song, “h-stability for nonlinear perturbed difference systems,” Bulletin of the Korean Mathematical Society, vol. 41, no. 3, pp. 435–450, 2004. [7] V. Lakshmikantham and S. G. Deo, Method of Variation of Parameters for Dynamic Systems, Series in Mathematical Analysis and Applications, Gordon and Breach Science Publishers, London, UK, 1998. [8] Z. F. Dong, Matrix Analysis, Harbin Industry University Publisher, Harbin, China, 2005. [9] S. K. Choi and N. J. Koo, “h-stability for nonlinear perturbed systems,” Annals of Differential Equations, vol. 11, no. 1, pp. 1–9, 1995. Abstract and Applied Analysis Advances in Operations Research Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Advances in Decision Sciences Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Mathematical Problems in Engineering Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Algebra Hindawi Publishing Corporation http://www.hindawi.com Probability and Statistics Volume 2014 The Scientific World Journal Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Differential Equations Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Volume 2014 Submit your manuscripts at http://www.hindawi.com International Journal of Advances in Combinatorics Hindawi Publishing Corporation http://www.hindawi.com Mathematical Physics Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Complex Analysis Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences Journal of Hindawi Publishing Corporation http://www.hindawi.com Stochastic Analysis Abstract and Applied Analysis Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com International Journal of Mathematics Volume 2014 Volume 2014 Discrete Dynamics in Nature and Society Volume 2014 Volume 2014 Journal of Journal of Discrete Mathematics Journal of Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Applied Mathematics Journal of Function Spaces Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Optimization Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014