Hindawi Publishing Corporation Advances in Difference Equations Volume 2009, Article ID 730484, 10 pages doi:10.1155/2009/730484 Research ArticleSolutionsof2nth-OrderBoundaryValueProblemforDifferenceEquationviaVariational Method Qingrong Zou and Peixuan Weng School of Mathematics, South China Normal University, Guangzhou 510631, China Correspondence should be addressed to Peixuan Weng, wengpx@scnu.edu.cn Received 7 July 2009; Accepted 15 October 2009 Recommended by Kanishka Perera The variational method and critical point theory are employed to investigate the existence ofsolutionsfor2nth-order difference equation Δ n p k−n Δ n y k−n −1 n1 fk, y k 0fork ∈ 1,N with boundaryvalue condition y 1−n y 2−n ··· y 0 0,y N1 ··· y Nn 0 by constructing a functional, which transforms the existence ofsolutionsof the boundaryvalueproblem BVP to the existence of critical points for the functional. Some criteria for the existence of at least one solution and two solutions are established which is the generalization for BVP of the even-order difference equations. Copyright q 2009 Q. Zou and P. Weng. 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. 1. Introduction Difference equations have been applied as models in vast areas such as finance insurance, biological populations, disease control, genetic study, physical field, and computer applica- tion technology. Because of their importance, many literature deals with its existence and uniqueness problems. For example, see 1–10. We notice that the existing results are usually obtained by various analytical techniques, for example, the conical shell fixed point theorem 1, 6, Banach contraction map method 7, Leray-Schauder fixed point theorem 2, 10, and the upper and lower solution method 3. It seems that the variational technique combining with the critical point theory 11 developed in the recent decades is one of the effective ways to study the boundaryvalue problems of difference equations. However because the variational method requires a “symmetrical” functional, it is hard for the odd-order difference equations to create a functional satisfying the “symmetrical” property. Therefore, the even-order difference equations have been investigated in most references. Let a, b, N > 1, n ≥ 1,k be integers, and a<b, a, b : {a, a 1, ,b} be a discrete interval in Z. Inspired by 5, 8, in this paper, we try to investigate the following 2nth-orderboundaryvalueproblem BVP of difference equationviavariational method combining 2 Advances in Difference Equations with some traditional analytical skills: Δ n p k−n Δ n y k−n −1 n1 f k, y k 0 k ∈ 1,N , 1.1 y 1−n y 2−n ··· y 0 0,y N1 ··· y Nn 0, 1.2 where Δ n y k Δ n−1 y k1 − Δ n−1 y k n 1 is the forward difference operator; p k ∈ R for k ∈ 1 −n, N and f ∈ C1,N × R, R. A variational functional for BVP 1.1-1.2 is constructed which transforms the existence ofsolutionsof the boundaryvalueproblem BVP to the existence of critical points of this functional. In order to prove the existence criteria of critical points of the functional, some lemmas are given in Section 2. Two criteria for the existence of at least one solution and two solutionsfor BVP 1.1-1.2 are established in Section 3 which is the generalization for BVP of the even-order difference equations. The existence results obtained in this paper are not found in the references, to the best of our knowledge. For convenience, we will use the following notations in the following sections: F k, u u 0 f k, s ds, p max k∈1−n,N p k ,p min k∈1−n,N p k . 1.3 2. Variational Structure and Preliminaries We need two lemmas from 12 or 11. Lemma 2.1. Let H be a real reflexive Banach space with a norm ·, and let φ be a weakly lower (upper) semicontinuous functional, such that lim x →∞ φ x ∞ or lim x →∞ φ x −∞ , 2.1 then there exists x 0 ∈ H such that φ x 0 inf x∈H φ x 0 or φ x 0 sup x∈H φ x 0 . 2.2 Furthermore, if φ has bounded linear G ˆ ateaux derivative, then φ x 0 0. Lemma 2.2 mountain-pass lemma. Let H be a real Banach space, and let φ : H → R be continuously differential, satisfying the P-S condition. Assume that x 0 ,x 1 ∈ H and Ω is an open neighborhood of x 0 ,butx 1 / ∈ Ω. If max{φx 0 ,φx 1 } < inf x∈∂Ω φx, then c inf h∈Γ max t∈0,1 φht is the critical valueof φ, where Γ { h | h : 0, 1 −→ H, h is continuous,h 0 x 0 ,h 1 x 1 } . 2.3 This means that there exists x 2 ∈ H,s.t.φ x 2 0, φx 2 c. The following lemma will be used in the proof of Lemma 2.4. Advances in Difference Equations 3 Lemma 2.3. If A m×m is a symmetric and positive-defined real matrix, B m×n is a real matrix, B T is the transposed matrix of B. Then B T AB is positive defined if and only if rank B n. Proof. Since A is positive defined, then B T AB is positive-defined ⇐⇒ ∀ x / 0,x T B T ABx > 0 ⇐⇒ ∀ x / 0, Bx T A Bx > 0 ⇐⇒ ∀ x / 0,Bx / 0 ⇐⇒ rank B n. 2.4 Let H be a Hilbert space defined by H y : 1 − n, N n −→ R | y 1−n y 2−n ··· y 0 0,y N1 ··· y Nn 0 2.5 with the norm y N k1 y 2 k ,y∈ H. 2.6 Hence H is an N-dimensional Hilbert space. For any q>1, let y q N k1 y 2 k 1/q , then one can show that there exist constants q 1 ,q 2 > 0, s.t. q 1 y y q q 2 y;thatis,· q is an equivalent norm of ·see 9, page 68. Lemma 2.4. There is λ x 2 N k1−n Δ n x k 2 4 n x 2 ,x∈ H, where λ is a postive constant . 2.7 Proof. Since x ∈ H, Δ n−j x N1 Δ n−j x j−n 0, j 1, 2, ,n.By using the inequality a − b 2 2a 2 b 2 , a, b ∈ R, we have N k1−n Δ n x k 2 N k1−n Δ n−1 x k1 − Δ n−1 x k 2 ≤ 2 N k1−n Δ n−1 x k1 2 Δ n−1 x k 2 2 N1 k2−n Δ n−1 x k 2 N k2−n Δ n−1 x k 2 4 N k2−n Δ n−1 x k 2 ≤ 4 × 2 N k2−n Δ n−2 x k1 2 N k2−n Δ n−2 x k 2 4 × 2 N1 k3−n Δ n−2 x k 2 N k2−n Δ n−2 x k 2 4 2 N k3−n Δ n−2 x k 2 . 2.8 4 Advances in Difference Equations Repeating the above process, we obtain N k1−n Δ n x k 2 4 n N k1 x k 2 4 n x 2 . 2.9 On the other hand, define b k Δ n x k n j0 −1 j C j n x kn−j , k ∈ 1 − n, N, where C j n is the combination number, then we can rewrite {b k } N 1−n in a vector form, that is, b Bx, where b b 1−n ,b 2−n , ,b N T , x x 1 ,x 2 , ,x N T ,and B ⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ 1 c 1 1 . . . . . . . . . c n c n−1 ··· 1 c n ··· c 1 1 . . . . . . . . . . . . c n c n−1 ··· 1 c n ··· c 1 1 . . . . . . . . . c n c n−1 c n ⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠ Nn×N , 2.10 where c i −1 i C i n . Hence rank B N. Note that N k1−n Δ n x k 2 b T b Bx T Bx x T B T Bx, 2.11 and by Lemma 2.3 with A m×m I Nn×Nn ,weknowthatB T B is positive defined. Hence all eigenvalues of B T B are real and positive. Let λ be the minimal eigenvalue of these N eigenvalues, then λ>0. Therefore x T B T Bx λx T x, that is, N 1−n Δ n x k 2 λx 2 . However, how to find the λ in Lemma 2.4 is a skillful and challenging task. The following lemma from 13 offers some help for the estimation of λ. Lemma 2.5 Brualdi 13. If A a ij ∈ M N is weak irreducible, then each eigenvalue is contained in the set γ∈CA ⎧ ⎨ ⎩ z ∈ C : P i ∈γ | z − a ii | P i ∈γ R i ⎫ ⎬ ⎭ . 2.12 Advances in Difference Equations 5 In Lemma 2.5, C is the complex number set, and the denotations CA, γ, P i , R i can be found in 13. Since B T B is positive defined, all eigenvalues are positive real numbers. Therefore, by Lemma 2.5,let B γ∈CB T B ⎧ ⎨ ⎩ z ∈ R : P i ∈γ | z − b ii | P i ∈γ R i ⎫ ⎬ ⎭ , 2.13 where B T B b ij . B is a subset of R and can be calculated directly from B T B. Define λ max{0, min{B}}. If λ>0, we can use this λ as λ in Lemma 2.4.Ifλ 0, then one needs to calculate the eigenvalues directly. Define the functional φ on H by φ y N k1−n 1 2 p k Δ n y k 2 − F k, y k . 2.14 Then φ is C 1 with φ y ,x N k1−n p k Δ n y k Δ n x k − x k f k, y k , 2.15 where x {x k } Nn k1−n ∈ H and ·, · is the inner product in H. In fact, we have φ y x − φ y N k1−n 1 2 p k Δ n y k Δ n x k 2 − Δ n y k 2 − F k, y k x k − F k, y k N k1−n p k Δ n y k Δ n x k 1 2 p k Δ n x k 2 − f k, y k θx k x k ,θ∈ 0, 1 . 2.16 The continuity of f and the right-hand side of the inequality in Lemma 2.4 lead to 2.15. Furthermore, for any x ∈ H, we have Δ n−j x N1 Δ n−j x 1−n 0, j 1, 2, ,n.By using the following formula e.g., see 14, page 28: n 2 kn 1 g k Δf k f k1 Δg k f k g k n 2 1 n 1 , 2.17 6 Advances in Difference Equations we have N 1−n p k Δ n y k Δ n x k p k−1 Δ n y k−1 Δ n−1 x k N1 1−n − N 1−n Δ p k−1 Δ n y k−1 Δ n−1 x k − N 1−n Δ p k−1 Δ n y k−1 Δ n−1 x k −Δ p k−2 Δ n y k−2 Δ n−2 x k N1 1−n N 1−n Δ 2 p k−2 Δ n y k−2 Δ n−2 x k N 1−n Δ 2 p k−2 Δ n y k−2 Δ n−2 x k . 2.18 Repeating the above process, we obtain N 1−n p k Δ n y k Δ n x k −1 n N 1−n Δ n p k−n Δ n y k−n x k . 2.19 Let φ y,x0, that is, N 1−n −1 n Δ n p k−n Δ n y k−n − f k, y k x k −1 n N 1−n Δ n p k−n Δ n y k−n −1 n1 f k, y k x k 0. 2.20 Since x ∈ H is arbitrary, we know that the solution of BVP 1.1-1.2 corresponds to the critical point of φ. 3. Main Results Now we present our main results of this paper. Theorem 3.1. If there exist M 1 > 0, a 1 > 0, a 2 ∈ R, and σ>2 s.t. F k, u a 1 | u | σ a 2 , ∀ | u | >M 1 , 3.1 then BVP 1.1-1.2 has at least one solution. Proof. In fact, we can choose a suitable a 2 < 0 such that F k, u a 1 | u | σ a 2 , ∀u ∈ R. 3.2 Advances in Difference Equations 7 Since there exists σ 1 > 0withσ 1 y y σ , we have N 1−n F k, y k a 1 N 1 y k σ a 2 N n a 1 σ σ 1 y σ a 2 N n . 3.3 Then by Lemma 2.4,weobtain φ y p 2 4 n y 2 − a 1 σ σ 1 y σ − a 2 N n . 3.4 Noticing that σ>2, we have lim y→∞ φy−∞. From Lemma 2.1 , the conclusion of this lemma follows. Corollary 3.2. If there exists M 2 > 0 s.t. ufk, u > 0 for all |u| >M 2 , and inf k∈1−n,N lim u →∞ f k, u | u | r r 1 , 3.5 where r, r 1 satisfy either r 1, r 1 > 4 n p or r>1,r 1 > 0,thenBVP1.1-1.2 has at least one solution. Proof. Assume that r 1, r 1 > 4 n p. Then for 1 r 1 − 4 n p/2 > 0, there exists M 3 >M 2 , such that |fk, y| r 1 − 1 |y| as |y| >M 3 . We have from the continuity of fk, u that there is a K>0 such that −K ≤ fk, u ≤ K for all k ∈ 1,N, |u|≤M 3 . When y>0, one has fk, y r 1 − 1 y>0fory ∈ M 3 , ∞, then y 0 f k, s ds M 3 0 f k, s ds y M 3 f k, s ds −KM 3 r 1 − 1 2 y 2 − r 1 − 1 2 M 2 3 ; 3.6 when y<0, one has fk, y r 1 − 1 y<0fory ∈ −∞, −M 3 , then y 0 f k, s ds −M 3 0 f k, s ds y −M 3 f k, s ds −KM 3 r 1 − 1 2 y 2 − r 1 − 1 2 M 2 3 . 3.7 Let c : −KM 3 − r 1 − 1 /2M 2 3 , then we have y 0 fk, sds r 1 − 1 /2y 2 c for y ∈ R. Therefore, we have φ y p 2 4 n y 2 − r 1 − 1 2 N 1 y k 2 − c 4 n p − r 1 1 2 y 2 − c − 1 2 y 2 − c, 3.8 which implies lim y→∞ φy−∞, and by Lemma 2.1, the conclusion of this lemma follows. Assume that r>1, r 1 > 0. Then for 2 r 1 /2 > 0, there exists M 4 >M 2 , such that |fk, y| r 1 /2|y| as |y| >M 4 . We have from the continuity of fk, u that there is 8 Advances in Difference Equations a K>0 such that −K ≤ fk, u ≤ K for all k ∈ 1,N, |u|≤M 4 . When y>0, one has fk, y r 1 /2y r > 0, y ∈ M 4 , ∞, then we have y 0 f k, s ds M 4 0 f k, s ds y M 4 f k, s ds − KM 4 r 1 2 r 1 y r1 − r 1 2 r 1 M r1 4 , 3.9 when y<0, one has fk, y −r 1 /2|y| r −r 1 /2−y r < 0, y ∈ −∞, −M 4 , then we have y 0 f k, s ds −M 4 0 f k, s ds y −M 4 f k, s ds − KM 4 r 1 2 y −M 4 −s r d −s − KM 4 r 1 2 r 1 y r1 − r 1 2 r 1 M 4 r1 . 3.10 Let d : − KM 4 − r 1 /2r 1M r1 4 , then we have y 0 fk, sds r 1 /2r 1|y| r1 d for |y| >M 4 . Therefore, by Theorem 3.1, the conclusion of this lemma follows. Theorem 3.3. Assume that p k > 0, k 1 − n, ,N,and i sup k∈1−n,N lim u → 0 fk, u/u r 2 <pλ, λ>0 is defined in Lemma 2.4; ii F satisfies 3.1 in Theorem 3.1 or f satisfies the assumptions in Corollary 3.2. Then BVP 1.1-1.2 has at least two solutions. Proof. We first show that φ satisfies the P-S condition. Let {y m } ∞ m1 ⊂ H satisfy that {φy m } is bounded and lim m →∞ φ y m 0. If {y m } is unbounded, it possesses a divergent subseries, say y m k → ∞ as k →∞. However from ii,weget3.4 or 3.8, hence φy m k →−∞as k →∞, which is contradictory to the the fact that {φy m } is bounded. Next we use the mountain-pass lemma to finish the proof. By i,for 3 pλ −r 2 /2 > 0, there exists R 1 > 0 such that fk, y/y r 2 3 for |y| R 1 . Then y 0 fk, sds r 2 3 /2y 2 for |y| R 1 . Now together with Lemma 2.3, we have φ y p 2 λ y 2 − r 2 3 2 N 1−n |y k | 2 y 2 p λ − r 2 − 3 2 3 2 y 2 > 0for y R 1 , 3.11 which implies that φ y 3 2 R 2 1 > 0 φ θ ,y∈ ∂Ω, 3.12 where θ is the zero element in H,andΩ{y ∈ H |y <R 1 }. Since we have from 3.4 or 3.8 that lim y→∞ φy−∞, there exists y 1 ∈ H with y 1 >R 1 , that is, y 1 / ∈ Ω, but Advances in Difference Equations 9 φy 1 <φθ0. Using Lemma 2.2, we have shown that ξ inf h∈Γ max t∈0,1 φht is the critical valueof φ, with Γ defined as Γ h | h : 0, 1 −→ H, h is continuous,h 0 θ, h 1 y 1 . 3.13 We denote y as its corresponding critical point. On the other hand, by Theorem 3.1 or Corollary 3.2, we know that there exists y ∗ ∈ H, s.t. φy ∗ sup y∈H φy. If y ∗ / y, the theorem is proved. If on the contrary, y ∗ y,that is, sup y∈H φyinf h∈Γ max t∈0,1 φht, that implies for any h ∈ Γ, max t∈0,1 φht sup y∈H φy. Taking h 1 / h 2 in Γ with max t∈0,1 φh 1 t max t∈0,1 φh 2 t sup y∈H φy, by the continuity of φht, there exist t 1 ,t 2 ∈ 0, 1 s.t. φh 1 t 1 max t∈0,1 φh 1 t, φh 2 t 2 max t∈0,1 φh 2 t. Hence h 1 t 1 , h 2 t 2 are two different critical points of φ, that is, BVP 1.1-1.2 has at least two different solutions. 4. An Example Consider the 6th-order boundaryvalueproblemfor difference equation Δ 6 y k−3 y 3 k e y 2 k −9 0,k∈ 1, 300 , y −2 y −1 y 0 0,y 301 y 302 y 303 0. 4.1 Let fk, uu 3 e u 2 −9 , we have lim u → 0 fk, u/u0, lim u →∞ fk, u/u∞. Hence fk, u satisfies the conditions in Theorem 3.3, the boundaryvalueproblem 4.1 has at least two solutions. Acknowledgments This research is partially supported by the NSF of China and NSF of Guangdong Province. References 1 R. P. Agarwal and J. Henderson, “Positive solutions and nonlinear eigenvalue problems for third- order difference equations,” Computers & Mathematics with Applications, vol. 36, no. 10–12, pp. 347–355, 1998. 2 R. P. Agarwal and D. O’Regan, “Singular discrete n, p boundaryvalue problems,” Applied Mathematics Letters, vol. 12, no. 8, pp. 113–119, 1999. 3 R. P. Agarwal and F H. Wong, “Upper and lower solutions method for higher-order discrete boundaryvalue problems,” Mathematical Inequalities & Applications, vol. 1, no. 4, pp. 551–557, 1998. 4 R. P. Agarwal, K. Perera, and D. O’Regan, “Multiple positive solutionsof singular and nonsingular discrete problems viavariational methods,” Nonlinear Analysis: Theory, Methods & Applications, vol. 58, no. 1-2, pp. 69–73, 2004. 5 Z. M. Guo and J. S. Yu, “Existence of periodic and subharmonic solutionsfor two-order superlinear difference equations,” Science in China Series A, vol. 33, pp. 226–235, 2003. 6 D. Jiang, J. Chu, D. O’Regan, and R. P. Agarwal, “Positive solutionsfor continuous and discrete boundaryvalue problems to the one-dimension p-Laplacian,” Mathematical Inequalities & Applications, vol. 7, no. 4, pp. 523–534, 2004. 7 L. T. Li and P. X. Weng, “Boundary value problems of second order functional difference equation,” Journal of South China Normal University Natural Science Edition, no. 3, pp. 20–24, 2003. 10 Advances in Difference Equations 8 H. H. Liang and P. X. Weng, “Existence and multiple solutionsfor a second-order difference boundaryvalueproblemvia critical point theory,” Journal of Mathematical Analysis and Applications, vol. 326, no. 1, pp. 511–520, 2007. 9 H. H. Liang and P. X. Weng, “Existence ofsolutionsfor a fourth-order difference boundaryvalueproblem and a critical point method,” Applied Mathematics A Journal of Chinese Universities, Series A, vol. 23, no. 1, pp. 67–72, 2008. 10 P. J. Y. Wong and R. P. Agarwal, “Existence theorems for a system of difference equations with n, p- type conditions,” Applied Mathematics and Computation, vol. 123, no. 3, pp. 389–407, 2001. 11 P. H. Rabinowitz, Minimax Methods in Critical Point Theory with Applications to Differential Equations, vol. 65, American Mathematical Society, Providence, RI, USA, 1986. 12 A. Ambrosetti and P. H. Rabinowitz, “Dual variational methods in critical point theory and applications,” Journal of Functional Analysis, vol. 14, pp. 349–381, 1973. 13 R. A. Horn and C. R. Johnson, Matrix Analysis, Cambridge University Press, Cambridge, UK, 1985. 14 M. Bohner and A. Peterson, Dynamic Equations on Time Scales: An Introduction with Application, Birkh ¨ auser, Boston, Mass, USA, 2001. . in Difference Equations Volume 2009, Article ID 730484, 10 pages doi:10.1155/2009/730484 Research Article Solutions of 2nth-Order Boundary Value Problem for Difference Equation via Variational. 1,N with boundary value condition y 1−n y 2−n ··· y 0 0,y N1 ··· y Nn 0 by constructing a functional, which transforms the existence of solutions of the boundary value problem. we try to investigate the following 2nth-order boundary value problem BVP of difference equation via variational method combining 2 Advances in Difference Equations with some traditional analytical