OSCILLATIONS OF FIRST ORDER DELAY AND ADVANCED DIFFERENCE EQUATIONS WITH VARIABLE ARGUMENTS by I.P. Stavroulakis Department of Mathematics University of Ioannina Email: [email protected] 1. Introduction The problem of establishing su¢ cient conditions for the oscillation of all solutions to the …rst-order delay di¤erence equation with constant arguments x(n) + p(n)x(n k) = 0; n 0 (E) has been the subject of many investigations. See, for example, [6, 8, 9, 12 17, 23, 26, 29, 34, 36, 37, 40, 43, 44, 48-58, 62, 64, 65] and the references cited therein. Recently this problem was also investigated for the delay di¤erence and the advanced di¤erence equation with variable arguments of the form x(n) + p(n)x( (n)) = 0, n 0 (E1 ) and rx(n) p(n)x( (n) = 0, n 1, [ x(n) p(n)x( (n) = 0, n 0]; (E2 ) where denotes the forward di¤erence operator x(n) = x(n + 1) x(n), r denotes the backward di¤erence operator rx(n) = x(n) x(n 1), fp(n)g is a sequence of nonnegative real numbers, f (n)g is a sequence of positive integers such that (n) n 1; for all n 0, and f (n)g [f (n)g] is a sequence of positive integers such that (n) n + 1 for all n 1, [ (n) n + 2 for all n 0] . See, for example, [1 5, 7, 10, 18, 26, 41, 42, 63] and the references cited therein. Strong interest in the equations (E1 ) and (E2 ) is motivated by the fact that they represent the discrete analogues of the delay x0 (t) + p(t)x( (t)) = 0, t t0 , (E1 )0 t t0 , (E2 )0 and the advanced di¤erential equation x0 (t) p(t)x( (t)) = 0, where p; ; 2 C([t0 ; 1); R+ ); R+ = [0; 1); (t); (t) are nondecreasing (t) < t and (t) > t for t t0 [see, for example, 11, 19-27, 30-33, 35, 38, 39, 45-47, 59-61]. 0 Key Words: Oscillation; delay, advanced di¤erence equations. 2010 Mathematics Subject Classi…cation: Primary 39A21, 39A10; Secondary 39A12. 1 2 2. Oscillation Criteria for Eq. (E1 )0 x0 (t) + p(t)x( (t)) = 0 1950, Myshkis lim sup[t t!1 (t)] < 1; lim inf [t (t)] lim inf p(t) > t!1 t!1 1972, Ladas, Lakshmikantham & Papadakis L := lim sup 1979 Ladas,1982 Koplatadze & Chanturija k := lim inf Rt (t) Rt (t) 1 e p(s)ds > 1 (C1 )0 p(s)ds > 1 e (C2 )0 In 1982 Ladas, S…cas and Stavroulakis and in 1984 Fukagai and Kusano established conditions (of the type (C1 )0 & (C2 )0 with oscillating coe¢ cient p (t) : 1988, Erbe & Zhang 1 e 0<k 1991 Jian Chao and L>1 1991 Kwong p1 (1 L> 1 is p 1 k L>1 1990 Elbert & Stavroulakis respectively, where k2 2(1 k) L>1 1992 Yu,Wang, Zhan & Qian k2 4 L>1 ln 1 2k k2 2 1 )2 1 +1 1 the smaller root of the equation 1998 Philos & S…cas L>1 1999 Jaroš & Stavroulakis L> ln k2 2(1 k) 1 +1 L> L > 2k + ln 1 p 1+ 5 2 0:966 (C4 )0 0:892 (C5 )0 0:863 (C6 )0 0:845 (C7 )0 0:735 =e . (C8 )0 p 1 k 1 2000 Kon,S…cas & Stavroulakis 2003 S…cas & Stavroulakis k2 2 (C3 )0 0:709 1 2k k2 2 (C9 )0 2 (C10 )0 0:471 (C11 )0 0:459 1 1 +2k 1 1 1, 0:599 It is to be noted that as k ! 0, then all the previous conditions (C3 )0 -(C10 )0 reduce to the condition (C1 )0 , i.e. L > 1. However our condition (C11 )0 leads to p L > 3 1 t 0:732 Example. Consider the delay di¤erential equation p 1 x0 (t) + px(t q sin2 t ) = 0; pe where p > 0, q > 0 and pq = 0:46 1e . Then k = 1e and L = 0:46. Thus, according to (C11 )0 , all solutions of this equation oscillate. Observe, however, that none of the conditions (C3 )0 -(C10 )0 is satis…ed for this equation. 3 3. Oscillation Criteria for Eq. (E) In this section we study the delay di¤erence equation with constant argument x(n) + p(n)x(n k) = 0; n = 0; 1; 2; :::: (E) where x(n) = x(n + 1) x(n); fp(n)g is a sequence of nonnegative real numbers and k is a positive integer. In 1981, Domshlak [12 ] was the …rst who studied this problem in the case where k = 1: Then, in 1989, Erbe and Zhang [23] established that all solutions of Eq.(E) are oscillatory if kk (2:1) lim inf p(n) > n!1 (k + 1)k+1 or n X lim sup p(i) > 1. (C1 ) n!1 i=n k In the same year, 1989, Ladas, Philos and S…cas [37]established the condition lim inf n!1 n X1 p(i) > i=n k k k+1 k+1 (C2 ) It is interesting to establish su¢ cient oscillation conditions for the equation (E) in the case where neither (C1 ) nor (C2 ) is satis…ed. In 1995, the following oscillation criterion was established by Stavroulakis [50]: Theorem 2.1 ([50]) Assume that 0 n X1 := lim inf n!1 k k+1 p(i) i=n k and k+1 2 0 lim sup p(n) > 1 (2:2) 4 n!1 then all solutions of Eq.(E) oscillate. In 2004, the same author [51] improved the condition (2.2) as follows: lim sup n!1 or n X1 i=n k lim sup n!1 p(i) > 1 n X1 p(i) > 1 2 0 (C3 ) 4 k 0 (2:3) i=n k In 2006, Chatzarakis and Stavroulakis [6], established the following condition lim sup n!1 n X1 i=n k p(i) > 1 2 0 2(2 0) Also, Chen and Yu [8] obtained the following oscillation condition p n 2 X 1 1 2 0 0 0 lim sup p (i) > 1 : 2 n!1 i=n k (2:4) (C5 ) 4 4. Oscillation Criteria for Eq. (E1 ) In this section we study the delay di¤erence equation with variable argument x(n) + p(n)x( (n)) = 0, n = 0; 1; 2; :::, (E1 ) where x(n) = x(n + 1) x(n); fp(n)g is a sequence of nonnegative real numbers and f (n)g is a nondecreasing sequence of integers such that (n) n 1 for all n 0 and limn!1 (n) = 1. In 2008, Chatzarakis, Koplatadze and Stavroulakis [2] investigated for the …rst time the oscillatory behaviour of Eq.(E1 ) in the case of a general delay argument (n) and derived the following theorem. Theorem 3.1 ([2]) If n X lim sup n!1 p(i) > 1 (D1 ) i= (n) then all solutions of Eq. (E1 ) oscillate. This result generalizes the oscillation criterion (C1 ): Also in the same year Chatzarakis, Koplatadze and Stavroulakis [3] extended the oscillation criterion (C2 ) to the general case of Eq. (E1 ). More precisely, the following theorem has been established in [3]. Theorem 3.2 ([3]) Assume that n X1 lim sup n!1 p(i) < +1 (3:1) i= (n) and n X1 := lim inf n!1 p(i) > i= (n) 1 : e (D2 ) Then all solutions of Eq.(E1 ) oscillate. Remark 3.1 It should be mantioned that in the case of the delay di¤erential equation x0 (t) + p(t)x( (t)) = 0, t t0 , (E1 )0 it has been proved (see [35,30]) that each one of the conditions lim sup n!1 Zt p(s)ds > 1 (C1 )0 1 : e (C2 )0 (t) or lim inf n!1 Zt p(s)ds > (t) 0 implies that all solutions of Eq.(E1 ) oscillate. Therefore, the conditions (D1 ) and (D2 ) are the discrete analogues of the conditions (C1 )0 and (C2 )0 and also the analogues of the conditions (C1 ) and (C2 ) in the case of a general delay argument (n): 5 As it has been mentioned above, it is interesting to …nd new su¢ cient conditions for the oscillation of all solutions of (E1 ); in the case where neither (D1 ) nor (D2 ) is satis…ed. In 2008, Chatzarakis, Koplatadze and Stavroulakis [2] and in 2008 and 2009, Chatzarakis, Philos and Stavroulakis [4] and [5] derived the following conditions: 1 e. Theorem 3.3 ([2,4,5]) (I) Assume that 0 < conditions: n X lim sup p (j) > 1 1 n!1 or lim sup n!1 or lim sup n!1 p (j) > 1 j= (n) p 1 1 2 p (j) > 1 j= (n) p 1 1 1 2 implies that all solutions of Eq.(E1 ) oscillate. 1 (II) If 0 < 1 e and in addition, p(n) lim sup n!1 or if 0 < 6 n!1 n X n X j= (n) p 1 p (j) > 1 j= (n) p 4 2 and in addition, p(n) lim sup 2 1 (3:2) j= (n) n X n X p Then either one of the p (j) > 1 1 2 4 3 2 p 1 p 1 2 (3:3) 2 2 (C5 ) for all large n; and 1 (3:4) 1 for all large n; and p 4 12 + 2 (3:5) then all solutions of Eq.(E1 ) are oscillatory. Remark 3.4 In the case where the sequence f (n)g is not assumed to be nondecreasing, de…ne (cf. [2, 3, 4, 5]) (n) = max f (s) : 0 s n; s 2 Ng . Clearly, the sequence of integers f (n)g is nondecreasing. In this case, Theorems 3.1, 3.2, 3.3, 3.4, and 3.5 can be formulated in a more general form. More precisely in the conditions (D1 ); (D2 ); (3:2); (3:3); (C6 )0 , (3:4) and (3:5) the term (n) is replaced by (n): 1 Remark 3.5 Observe the following:(i) When 0 < e , it is easy to verify that p p p 2 p 1 2 1 1 1 1 2 1 p > > > (1 1 )2 2 2 1 0 and therefore condition (C6 )p is weaker than the conditions (3.4), (3.3) and (3.2). (ii) When 0 < 6 4 2, it is easy to show that p p 1 1 2 2 3 4 12 + 2 > 1 1 2 4 2 and therefore in this case, (C6 )0 and espep inequality (3.5) improves the inequality 0 cially, when = 6 4 2 ' 0:3431457; the lower bound in (C6 ) is 0.8929094 while in (3.5) is 0.7573593. 6 5. Oscillation Criteria for Eq. (E2 ) In this section, we study the advanced di¤erence equation with variable argument rx(n) p(n)x( (n) = 0, n 1, [ x(n) p(n)x( (n) = 0, n 0]; (E2 ) where r denotes the backward di¤erence operator rx(n) = x(n) x(n 1), denotes the forward di¤erence operator x(n) = x(n + 1) x(n), fp(n)g is a sequence of nonnegative real numbers and f (n)g [f (n)g] is a sequence of positive integers such that (n) n + 1 for all n 1, [ (n) n + 2 for all n 0] . For Eq. (E2 ) very recently, Chatzarakis and Stavroulakis [7] established the following theorems: If Theorem 4.1 ([7]) Assume that the sequence f (n)g [f (n)g] is nondecreasing. lim sup n!1 (n) X i=n 2 3 (n) 1 p(i) 4lim sup n!1 then all solutions of Eq.(E2 ) oscillate. X p(i)5 > 1, i=n (A1 ) Theorem 4.2 ([7]) Assume that the sequence f (n)g [f (n)g] is nondecreasing, and 2 3 (n) (n) 1 X X lim inf p (i) 4lim inf p (i)5 = . (4:1) n!1 If 0 < n!1 i=n+1 i=n+1 1, and lim sup n!1 (n) X i=n 2 (n) 1 p(i) 4lim sup n!1 then all solutions of (E2 ) oscillate. If 0 < 1=2, and lim sup n!1 (n) X i=n 2 (n) 1 p(i) 4lim sup n!1 X i=n X i=n 3 p(i)5 > 1 3 p(i)5 > 1 then all solutions of (E2 ) oscillate. p If 0 < < (3 5 5)=2; and in addition p(n) 2 3 (n) (n) 1 X X lim sup p(i) 4lim sup p(i)5 > 1 n!1 n!1 i=n i=n p 1 p 1 1 2 1 p p 3 1 1 2 1 1 , 2 (4:3) for all large n, and 1 + 2 1 , p 4 2, and in addition p(n) for all large n; and 2 2 3 (n) (n) 1 p X X 1 4 lim sup p(i) lim sup p(i)5 > 1 2 3 4 12 + 4 n!1 n!1 i=n i=n or if 0 < (4:2) (4:4) 6 then all solutions of (E2 ) oscillate. 2 (4:5) 7 Remark 4.1. In the case where the sequence f (n)g [ (n)] is not assumed to be nondecreasing, de…ne (cf. [7]) (n) = max f (s) : 1 s n; s 2 Ng , [ (n) = max f (s) : 1 s n; s 2 Ng] . Clearly, the sequence of integers f (n)g [f (n)g] is nondecreasing. In this case, Theorems 4.1 and 4.2 can be formulated in a more general form. More precisely, in the conditions (A1 ); (4:2) (4:3), (4:4) and (4:5) the term (n) [ (n)] is replaced by (n) [ (n)] : Remark 4.2. 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