Electronic Journal of Differential Equations, Vol. 2010(2010), No. 146, pp. 1–7. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu EXISTENCE OF NON-OSCILLATORY SOLUTIONS FOR A HIGHER-ORDER NONLINEAR NEUTRAL DIFFERENCE EQUATION ZHENYU GUO, MIN LIU Abstract. This article concerns the solvability of the higher-order nonlinear neutral delay difference equation s “ ` ´” X ∆ akn . . . ∆ a2n ∆(a1n ∆(xn + bn xn−d )) + pjn fj (xn−rjn ) = qn , j=1 where n ≥ n0 ≥ 0, d, k, j, s are positive integers, fj : R → R and xfj (x) ≥ 0 for x 6= 0. Sufficient conditions for the existence of non-oscillatory solutions are established by using Krasnoselskii fixed point theorem. Five theorems are stated according to the range of the sequence {bn }. 1. Introduction and preliminaries Interest in the solvability of difference equations has increased lately, as inferred from the number of related publications; see for example the references in this article and their references. Authors have examined various types difference equations, as follows: n ≥ 0, in [14], ∆(an ∆xn ) = qn f (xn+1 ), n ≥ 0, in [11], (1.2) n ≥ n0 , in [6], (1.3) ∆(an ∆xn ) + pn xg(n) = 0, ∆(an ∆xn ) = qn xn+1 , 2 ∆ (xn + pxn−m ) + pn xn−k − qn xn−l = 0, 2 ∆ (xn + pxn−k ) + f (n, xn ) = 0, ∆2 (xn − pxn−τ ) = m X qi fi (xn−σi ), n ≥ 1, (1.1) in [10], n ≥ n0 , in [9], (1.4) (1.5) i=1 ∆(an ∆(xn + bxn−τ )) + f (n, xn−d1n , xn−d2n , . . . , xn−dkn ) = cn , n ≥ n0 , in [8], m (1.6) ∆ (xn + cxn−k ) + pn xn−r = 0, n ≥ n0 , m ∆ (xn + cn xn−k ) + pn f (xn−r ) = 0, n ≥ n0 , in [15], in [3, 4, 12, 13], 2000 Mathematics Subject Classification. 34K15, 34C10. Key words and phrases. Nonoscillatory solution; neutral difference equation; Krasnoselskii fixed point theorem. c 2010 Texas State University - San Marcos. Submitted July 30, 2010. Published October 14, 2010. 1 (1.7) (1.8) 2 Z. GUO, M. LIU, ∆m (xn + cxn−k ) + u X EJDE-2010/146 psn fs (xn−rs ) = qn , n ≥ n0 , in [16], (1.9) s=1 ∆m (xn + cxn−k ) + pn xn−r − qn xn−l = 0, n ≥ n0 , in [17]. (1.10) Motivated by the above publications, we investigate the higher-order nonlinear neutral difference equation s X ∆ akn . . . ∆ a2n ∆(a1n ∆(xn + bn xn−d )) + pjn fj (xn−rjn ) = qn , (1.11) j=1 where n ≥ n0 ≥ 0, d, k, j, s are positive integers, {ain }n≥n0 (i = 1, 2, . . . , k), {bn }n≥n0 , {pjn }n≥n0 (1 ≤ j ≤ s) and {qn }n≥n0 are sequences of real numbers, rjn ∈ Z (1 ≤ j ≤ s, n0 ≤ n), fj : R → R and xfj (x) ≥ 0 for x 6= 0 (j = 1, 2, . . . , s). Clearly, difference equations (1.1)–(1.10) are special cases of (1.11), for which we use Krasnoselskii fixed point theorem to obtain non-oscillatory solutions. Lemma 1.1 (Krasnoselskii Fixed Point Theorem). Let Ω be a bounded closed convex subset of a Banach space X and T1 , T2 : S → X satisfy T1 x + T2 y ∈ Ω for each x, y ∈ Ω. If T1 is a contraction mapping and T2 is a completely continuous mapping, then the equation T1 x + T2 x = x has at least one solution in Ω. As usual, the forward difference ∆ is defined as ∆xn = xn+1 − xn , and for a positive integer m the higher-order difference is defined as ∆m xn = ∆(∆m−1 xn ), ∆0 xn = xn . In this article, R = (−∞, +∞), N is the set of positive integers, Z is the sets of all integers, α = inf{n − rjn : 1 ≤ j ≤ s, n0 ≤ n}, β = min{n0 − d, α}, limn→∞ (n − rjn ) = +∞, 1 ≤ j ≤ s, lβ∞ denotes the set of real-valued bounded sequences x = {xn }n≥β . It is well known that lβ∞ is a Banach space under the supremum norm kxk = supn≥β |xn |. For N > M > 0, let A(M, N ) = x = {xn }n≥β ∈ lβ∞ : M ≤ xn ≤ N, n ≥ β . Obviously, A(M, N ) is a bounded closed and convex subset of lβ∞ . Put b = lim sup bn and b = lim inf bn . n→∞ n→∞ lβ∞ Definition 1.2 ([5]). A set Ω of sequences in is uniformly Cauchy (or equiCauchy) if for every ε > 0, there exists an integer N0 such that |xi − xj | < ε, whenever i, j > N0 for any x = xk in Ω. Lemma 1.3 (Discrete Arzela-Ascoli’s theorem [5]). A bounded, uniformly Cauchy subset Ω of lβ∞ is relatively compact. By a solution of (1.11), we mean a sequence {xn }n≥β with a positive integer N0 ≥ n0 + d + |α| such that (1.11) is satisfied for all n ≥ N0 . As is customary, a solution of (1.11) is said to be oscillatory about zero, or simply oscillatory, if the terms xn of the sequence {xn }n≥β are neither eventually all positive nor eventually all negative. Otherwise, the solution is called non-oscillatory. EJDE-2010/146 EXISTENCE OF NON-OSCILLATORY SOLUTIONS 3 2. Existence of non-oscillatory solutions In this section, we will give five sufficient conditions of the existence of nonoscillatory solutions of (1.11). Theorem 2.1. If there exist constants M and N with N > M > 0 and such that |bn | ≤ b < ∞ X max t=n0 N −M , 2N eventually, (2.1) 1 , |pjt |, |qt | : 1 ≤ i ≤ k, 1 ≤ j ≤ s < +∞, |ait | (2.2) then (1.11) has a non-oscillatory solution in A(M, N ). Proof. Choose L ∈ (M + bN, N − bN ). By (2.1) and (2.2), an integer N0 > n0 + d + |α| can be chosen such that |bn | ≤ b < N −M , ∀n ≥ N0 , 2N (2.3) and ∞ ∞ X X t1 =N0 t2 =t1 ··· ∞ X Ps ∞ X F j=1 pjt + |qt | ≤ min{L − bN − M, N − bN − L}, Qk aiti tk =tk−1 t=tk i=1 (2.4) where F = maxM ≤x≤N {fj (x) : 1 ≤ j ≤ s}. Define two mappings T1 , T2 : A(M, N ) → X by ( L − bn xn−d , n ≥ N0 , (T1 x)n = (2.5) (T1 x)N0 , β ≤ n < N0 , P∞ P∞ (−1)k t1 =n t2 =t1 . . . P P∞ Psj=1 pjt fj (xt−rjt )−qt ∞ Qk (2.6) (T2 x)n = , n ≥ N0 , tk =tk−1 t=tk i=1 aiti (T2 x)N0 , β ≤ n < N0 , for all x ∈ A(M, N ). (i) Note that T1 x + T2 y ∈ A(M, N ) for all x, y ∈ A(M, N ). In fact, for every x, y ∈ A(M, N ) and n ≥ N0 , by (2.4), we have ∞ X ∞ ∞ ∞ Ps X X X j=1 pjt fj (yt−rjt ) − qt (T1 x + T2 y)n ≥ L − bN − ··· Qk t1 =n t2 =t1 tk =tk−1 t=tk i=1 aiti P s ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | ≥ L − bN − ··· ≥M Qk aiti t1 =N0 t2 =t1 tk =tk−1 t=tk i=1 and (T1 x + T2 y)n ≤ L + bN + ∞ ∞ X X ··· t1 =N0 t2 =t1 ≤ N. That is, (T1 x + T2 y)(A(M, N )) ⊆ A(M, N ). ∞ X Ps ∞ X F j=1 pjt + |qt | Qk aiti tk =tk−1 t=tk i=1 4 Z. GUO, M. LIU, EJDE-2010/146 (ii) W show that T1 is a contraction mapping on A(M, N ). For any x, y ∈ A(M, N ) and n ≥ N0 , it is easy to derive that (T1 x)n − (T1 y)n ≤ |bn kxn−d − yn−d | ≤ bkx − yk, which implies kT1 x − T1 yk ≤ bkx − yk. −M Then b < N2N < 1 ensures that T1 is a contraction mapping on A(M, N ). (iii) We show that T2 is completely continuous. First, we show T2 that is contin(u) (u) uous. Let x(u) = {xn } ∈ A(M, N ) be a sequence such that xn → xn as u → ∞. Since A(M, N ) is closed, x = {xn } ∈ A(M, N ). Then, for n ≥ N0 , (u) ∞ ∞ ∞ ∞ Ps fj (xt−r X X X X p ) − fj (xt−rjt )| jt j=1 jt T2 x(u) . ··· Qk n − T2 xn ≤ tk =tk−1 t=tk i=1 aiti t1 =N0 t2 =t1 Since Ps j=1 Ps (u) (u) pjt fj (xt−rjt ) − fj (xt−rjt )| j=1 pjt |fj (xt−rjt )| + |fj (xt−rjt )| ≤ Qk Qk i=1 aiti i=1 aiti Ps 2F j=1 pjt ≤ Qk ait i=1 i (u) |fj (xt−rjt ) − fj (xt−rjt )| → 0 as u → ∞ for j = 1, 2, . . . , s, it follows from (2.2) and and the Lebesgue dominated convergence theorem that limu→∞ kT2 x(u) −T2 xk = 0, which means that T2 is continuous. Next, we show that T2 A(M, N ) is relatively compact. By (2.2), for any ε > 0, take N1 ≥ N0 large enough, Ps ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | ε ··· < . (2.7) Qk 2 tk =tk−1 t=tk i=1 aiti t1 =N1 t2 =t1 Then, for any x = {xn } ∈ A(M, N ) and n1 , n2 ≥ N1 , (2.7) ensures that ∞ ∞ ∞ Ps ∞ X X X X j=1 pjt fj (yt−rjt ) − qt T2 xn1 − T2 xn2 ≤ ··· Qk t1 =n1 t2 =t1 tk =tk−1 t=tk i=1 aiti ∞ ∞ ∞ ∞ Ps X X X X j=1 pjt fj (yt−rjt ) − qt + ··· Qk t1 =n2 t2 =t1 tk =tk−1 t=tk i=1 aiti P s ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | ≤ ··· Qk tk =tk−1 t=tk i=1 aiti t1 =N1 t2 =t1 P s ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | + ··· Qk aiti t1 =N1 t2 =t1 tk =tk−1 t=tk i=1 ε ε < + = ε, 2 2 which implies T2 A(M, N ) begin uniformly Cauchy. Therefore, by Lemma 1.3, the set T2 A(M, N ) is relatively compact. By Lemma 1.1, there exists x = {xn } ∈ A(M, N ) such that T1 x + T2 x = x, which is a bounded non-oscillatory solution to (1.11). This completes the proof. EJDE-2010/146 EXISTENCE OF NON-OSCILLATORY SOLUTIONS 5 Theorem 2.2. If (2.2) holds, bn ≥ 0 eventually, 0 ≤ b ≤ b < 1, 2−b M 1−b and there exist constants M and N with N > oscillatory solution in A(M, N ). (2.8) > 0 then (1.11) has a non- b Proof. Choose L ∈ (M + 1+b 2 N, N + 2 M ). By (2.2) and (2.8), an integer N0 > n0 + d + |α| can be chosen such that and 1+b b ≤ bn ≤ , ∀n ≥ N0 2 2 Ps ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | ··· Qk aiti (2.9) t1 =N0 t2 =t1 tk =tk−1 t=tk i=1 (2.10) n b o 1+b N, N − L + M , ≤ min L − M − 2 2 where F = maxM ≤x≤N {fj (x) : 1 ≤ j ≤ s}. Then define T1 , T2 : A(M, N ) → X as (2.5) and (2.6). The rest proof is similar to that of Theorem 2.1, and it is omitted. Theorem 2.3. If (2.2) holds, bn ≤ 0 eventually, −1 < b ≤ b ≤ 0, and there exist constants M and N with N > oscillatory solution in A(M, N ). 2+b 1+b M (2.11) > 0, then (1.11) has a non- 1+b Proof. Choose L ∈ ( 2+b 2 M, 2 N ). By (2.2) and (2.11), an integer N0 > n0 +d+|α| can be chosen such that b−1 b ≤ bn ≤ , ∀n ≥ N0 , (2.12) 2 2 and Ps ∞ ∞ ∞ ∞ X X X X F j=1 pjt + |qt | ··· Qk tk =tk−1 t=tk i=1 aiti t1 =N0 t2 =t1 (2.13) n o 2+b 1+b ≤ min L − M, N −L , 2 2 where F = maxM ≤x≤N {fj (x) : 1 ≤ j ≤ s}. Then define T1 , T2 : A(M, N ) → X by (2.5) and (2.6). The rest proof is similar to that of Theorem 2.1, and is omitted. Theorem 2.4. If (2.2) holds, bn > 1 eventually, 1 < b, and b < b2 < +∞, (2.14) 2 and there exist constants M and N with N > non-oscillatory solution in A(M, N ). b(b −b) M b(b2 −b) > 0, then (1.11) has a Proof. Take ε ∈ (0, b − 1) sufficiently small satisfying 1 < b − ε < b + ε < (b − ε)2 (2.15) and (b + ε)(b − ε)2 − (b + ε)2 N > (b + ε)2 (b − ε) − (b − ε)2 M. (2.16) 6 Z. GUO, M. LIU, EJDE-2010/146 b+ε M . By (2.2) and (2.15), an integer Choose L ∈ (b + ε)M + b−ε N, (b − ε)N + b−ε b+ε N0 > n0 + d + |α| can be chosen such that b − ε < bn < b + ε, ∀b ≥ N0 (2.17) and ∞ ∞ X X ∞ X ··· t1 =N0 t2 =t1 Ps ∞ X F j=1 pjt + |qt | Qk aiti tk =tk−1 t=tk i=1 (2.18) o b−ε L − (b − ε)M − N, M + (b − ε)N − L , ≤ min b+ε b+ε nb − ε where F = maxM ≤x≤N {fj (x) : 1 ≤ j ≤ s}. Define two mappings T1 , T2 : A(M, N ) → X by ( L n+d − xbn+d , n ≥ N0 , (2.19) (T1 x)n = bn+d (T1 x)N0 , β ≤ n < N0 , (−1)k P∞ P∞ t1 =n t2 =t1 . . . bn+d P P∞ Psj=1 pjt fj (xt−rjt )−qt ∞ Qk T2 x)n = (2.20) , n ≥ N0 , tk =tk−1 t=tk i=1 aiti (T2 x)N0 , β ≤ n < N0 , for all x ∈ A(M, N ). The rest proof is similar to that in Theorem 2.1, and is omitted. Theorem 2.5. If (2.2) holds, bn < −1 eventually, −∞ < b, b < −1 (2.21) 1+b M 1+b and there exist constants M and N with N > > 0, then (1.11) has a nonoscillatory solution in A(M, N ). Proof. Take ∈ 0, −(1 + b) sufficiently small satisfying b − < b + < −1 (2.22) and (2.23) (1 + b + )N < (1 + b − )M. Choose L ∈ (1 + b + )N, (1 + b − )M . By (2.2) and (2.22), an integer N0 > n0 + d + |α| can be chosen such that b − < bn < b + , and ∞ ∞ X X t1 =N0 t2 =t1 ··· ∞ X ∀n ≥ N0 , Ps ∞ X F j=1 pjt + |qt | Qk aiti (2.24) tk =tk−1 t=tk i=1 (2.25) o n b+ b+ ≤ min b + + M− L, L − (1 + b + )N , b− b− where F = maxM ≤x≤N {fj (x) : 1 ≤ j ≤ s}. Then define T1 , T2 : A(M, N ) → X as (2.19) and (2.20). The rest proof is similar to that in Theorem 2.1, and is omitted. EJDE-2010/146 EXISTENCE OF NON-OSCILLATORY SOLUTIONS 7 Remark 2.6. Theorems 2.1–2.5 extend the results in Cheng [6, Theorem 1], Liu, Xu and Kang [8, Theorems 2.3-2.7], Zhou and Huang [16, Theorems 1-5] and corresponding theorems in [3, 4, 9, 10, 11, 12, 13, 14, 15]. Acknowledgments. The authors are grateful to the anonymous referees for their careful reading, editing, and valuable comments and suggestions. References [1] R. P. Agarwal; Difference equations and inequalities, 2nd ed., Dekker, New York (2000). [2] R. P. Agarwal, S. R. Grace, D. O’Regan; Oscillation theory for difference and functional differential equations, Kulwer Academic (2000). [3] R. P. Agarwal, E. Thandapani, P. J. Y. Wong; Oscillations of higher-order neutral difference equations, Appl. Math. Lett. 10 (1997), 71–78. [4] R. P. Agarwal, S. R. Grace; The oscillation of higher-order nonlinear difference equations of neutral type, JAppl. Math. Lett. 12 (1999), 77–83. [5] S. S. Cheng, W. T. Patula; An existence theorem for a nonlinear difference equation, Nonlinear Anal.20 (1993), 193–203. [6] J. F. Cheng; Existence of a nonoscillatory solution of a second-order linear neutral difference equation, Appl. Math. Lett. 20 (2007), 892–899. [7] I. Gyori and G. Ladas; Oscillation theory for delay differential equations with applications, Oxford Univ. Press, London (1991). [8] Z. Liu, Y. Xu, S. M. Kang; Global solvability for a second order nonlinear neutral delay difference equation, Comput. Math. Appl. 57 (2009), 587–595. [9] Q. Meng, J. Yan, Bounded oscillation for second-order nonlinear difference equations in critical and non-critical states, J. Comput. Appl. Math. 211 (2008), 156–172 [10] M. Migda, J. Migda; Asymptotic properties of solutions of second-order neutral difference equations, Nonlinear Anal. 63 (2005), 789–799. [11] E. Thandapani, M. M. S. Manuel, J. R. Graef, P. W. Spikes; Monotone properties of certain classes of solutions of second-order difference equations, Comput. Math. Appl. 36 (2001), 291–297. [12] F. Yang, J. Liu; Positive solution of even order nonlinear neutral difference equations with variable delay, J. Systems Sci. Math. Sci. 22 (2002), 85–89. [13] B. G. Zhang, B. Yang; Oscillation of higher order linear difference equation, Chinese Ann. Math. 20 (1999), 71–80. [14] Z. G. Zhang, Q. L. Li; Oscillation theorems for second-order advanced functional difference equations, Comput. Math. Appl. 36 (1998), 11–18. [15] Y. Zhou; Existence of nonoscillatory solutions of higher-order neutral difference equations with general coefficients, Appl. Math. Lett. 15 (2002), 785–791. [16] Y. Zhou, Y. Q. Huang; Existence for nonoscillatory solutions of higher-order nonlinear neutral difference equations, J. Math. Anal. Appl. 280 (2003), 63–76. [17] Y. Zhou, B. G. Zhang; Existence of nonoscillatory solutions of higher-order neutral delay difference equations with variable coefficients, Comput. Math. Appl. 45 (2003), 991–1000. Zhenyu Guo School of Sciences, Liaoning Shihua University, Fushun, Liaoning 113001, China E-mail address: guozy@163.com Min Liu School of Sciences, Liaoning Shihua University, Fushun, Liaoning 113001, China E-mail address: min liu@yeah.net