Oscillation Criteria for Second-Order Neutral Delay Dynamic Equations with Nonlinearities Given by Riemann-Stieltjes Integrals
Abstract
We establish several oscillation criteria for a class of second-order neutral delay dynamic equations with nonlinearities given by Riemann-Stieltjes integrals. Our results extend and unify a number of other existing results and handle the cases which are not covered by known criteria. The new results we obtain are of significance because the equations we study allow an infinite number of nonlinear terms and even a continuum of nonlinearities.
1. Introduction
-
(H1) a, b ∈ 𝕋1, 𝕋1 is another time scale, Crd (𝔻, 𝕊) denotes the collection of all functions f : 𝔻 → 𝕊 which are right-dense continuous on 𝔻;
-
(H2) r(t) ∈ Crd ([t0, ∞) 𝕋, (0, ∞)), , lim t→∞R(t, t0) = ∞, p(t) ∈ Crd ([t0, ∞) 𝕋, [0,1)), is a strictly increasing and satisfying 0 < θ(a) < α < θ(b), ;
-
(H3) τ(t) ∈ Crd ([t0, ∞) 𝕋, [t0, ∞) 𝕋), τ(t) ⩽ t, for t ∈ [t0, ∞) 𝕋, lim t→∞τ(t) = ∞, δ(t) ∈ Crd ([t0, ∞) 𝕋, [t0, ∞) 𝕋), δ(t) ⩽ t, for t ∈ [t0, ∞) 𝕋, lim t→∞δ(t) = ∞, , lim t→∞g(t, s) = ∞ for any ;
-
(H4) δΔ(t) > 0 is right-dense continuous on [t0, ∞) 𝕋, and δ(σ(t)) = σ(δ(t)) for all t ∈ [t0, ∞) 𝕋, where σ(t) is the forward jump operator on [t0, ∞) 𝕋;
-
(H5) f(t, u) ∈ C([t0, ∞) 𝕋 × ℝ, ℝ) is a continuous function such that uf(t, u) > 0, for all u ≠ 0 and there exists a positive right-dense continuous function q(t) defined on [t0, ∞) 𝕋 such that |f(t, u)|⩾q(t) | uα| for all t ∈ [t0, ∞) 𝕋 and for all u ∈ ℝ;
-
(H6) is strictly increasing; denotes the Riemann-Stieltjes integral of the function f on with respect to ξ.
By a solution of (1), we mean a function x(t) such that and , tx⩾t0 and satisfying (1) for all t⩾tx, where denotes the set of right-dense continuously Δ-differentiable functions on (tx, ∞) 𝕋. In the sequel, we will restrict our attention to those solutions of (1) which exist on the half-line [tx, ∞) 𝕋 and satisfy for any . A nontrivial solution of (1) is called oscillatory if it has arbitrary large zeros; otherwise, it is called nonoscillatory. Equation (1) is said to be oscillatory if all its solutions are oscillatory.
In recent years, there has been much research activity concerning the oscillation and nonoscillation of solutions of neutral functional equations on time scales, and we refer the reader to the papers [1–10] and the references cited therein. For an introduction to time scale calculus and dynamic equations, we refer the reader to the landmark paper of Hilger [11] and the seminal book by Bohner and Peterson [12] for a comprehensive treatment of the subject.
It is obvious that (2)–(4) are special cases of (1). In the present paper, we will establish several oscillation criteria for the more general (1), which is of significance because (1) allows an infinite number of nonlinear terms and even a continuum of nonlinearities determined by the function ξ. Our results extend and unify a number of other existing results and handle the cases which are not covered by known criteria. Finally, two examples are demonstrated to illustrate the efficiency of our work.
2. Preliminaries
In the sequel, we denote by Lξ[a, b] the set of Riemann-Stieltjes integrable functions on with respect to ξ, and we use the convention that ln 0 = −∞, e−∞ = 0.
Lemma 1 (see [15].)Suppose that (H4) holds. Let x : 𝕋 → ℝ. If xΔ exists for all sufficiently large t ∈ 𝕋, then (x(δ(t))) Δ = xΔ(δ(t))δΔ(t) for all sufficiently large t ∈ 𝕋.
Lemma 2 (see [12].)Assume that x(t) is Δ-differentiable and eventually positive or eventually negative, then
Lemma 3 (see [16].)Suppose that X and Y are nonnegative, then
Lemma 5 (see [17].)Let τ(t) ∈ Crd([t0, ∞) 𝕋, [t0, ∞) 𝕋) satisfying 0 ⩽ τ(t) ⩽ t, and . Assume such that r(t) | xΔ(t)|α−1xΔ(t) is nonincreasing on [t0, ∞) 𝕋, where r(t) ∈ Crd([t0, ∞) 𝕋, (0, ∞)), α > 0 is a constant. Then,
3. Main Results
Theorem 6. Assume that (H1)–(H6) hold. If there exist a function and a function η(s) ∈ Lξ[a, b] such that η(s) > 0 on ,
Proof. Suppose that (1) has a nonoscillatory solution x(t), then there exists T0 (∈𝕋)⩾t0 such that x(t) ≠ 0 for all t ∈ [T0, ∞) 𝕋. Without loss of generality, we assume that x(t) > 0, x(τ(t)) > 0, x(δ(t)) > 0, and x(g(t, s)) > 0 for t ∈ [T0, ∞) 𝕋, , because a similar analysis holds for x(t) < 0, x(τ(t)) < 0, x(δ(t)) < 0, and x(g(t, s)) < 0. Then, from (1), (H2), and (H5), we get
We claim that
We choose some T1 (∈𝕋)⩾T0 such that δ(t)⩾T0 for t ∈ [T1, ∞) 𝕋. Therefore, from (14), (15), and the fact δ(t) ⩽ σ(t), we have that
Define
In the first case, α⩾1. By (15), (H4), and Lemmas 1 and 2, we have
In the second case, 0 < α < 1. By (15), (H4), and Lemmas 1 and 2, we get
Taking
Remark 7. If we take r(x, s) = 0 and use the convention that ln 0 = −∞, e−∞ = 0, then Theorems 6 reduces to [15, Theorems 3.1]. If furthermore α⩾1 is a quotient of odd positive integer, then Theorem 6 reduces to [14, Theorem 3.1].
Remark 8. The function η(t) satisfying (10) and (11) in Theorem 6 can be constructed explicitly for any nondecreasing function ξ. In fact, if we assume that , and let ,
Moreover,
Remark 9. Set 𝕋1 = ℕ, a = 1, b = n for n ∈ ℕ, and
-
ξ(s) = s;
-
θ(s) = βs, (s = 1,2, …, n) satisfying β1 > β2 > ⋯>βm > α > βm+1 > ⋯>βn;
-
k(t, s) = qs(t), s = 1,2, …, n;
-
g(t, s) = τs(t), s = 1,2, …, n;
Next, we use the general weighted functions from the class Ϝ which will be extensively used in the sequel.
Let 𝔻 ≡ {(t, s)∈[t0, ∞) 𝕋 × [t0, ∞) 𝕋 : t⩾s⩾t0}, we say that a continuous function H(t, s) ∈ Crd (𝔻, ℝ) belongs to the class Ϝ if
- (i)
H(t, t) = 0 for t ∈ [t0, ∞) 𝕋 and H(t, s) > 0 for t > s⩾t0 where t, s ∈ [t0, ∞) 𝕋;
- (ii)
H(t, s) has a nonpositive right-dense continuous Δ-partial derivative with respect to the second variable.
Theorem 10. Assume that (H1)–(H6) hold. If there exist functions H(t, s) ∈ Ϝ, , η(t) ∈ Lξ[a, b] such that η(s) > 0 on , (10) and (11) hold, and
Proof. We proceed as in the proof of Theorem 6 to have (35). From (35), we obtain
Taking
Then, it follows that
Therefore,
Remark 11. In the literature, there are so many results for second-order nonlinear neutral functional dynamic equation; however, to the best of our knowledge, there is no work done attempting to study the neutral functional dynamic equation with an infinite number of nonlinear terms. Hence, our paper seems to be the first one dealing with this untouched problem. Our results not only unify the existing results in the literature, but also extend the existing results to a wider class of dynamic equations.
4. Examples
Example 1. Consider the following dynamic equation:
If and , δ(t) = t/q0, g(t, s) = q0t, and , where k0 is an arbitrary positive integer, then δΔ(t) = 1/q0. We can choose η(t) = 1, ϕ(t) = t. Then, it is easy to get that M(t) = 1/t, and therefore,
Example 2. Consider on 𝕋 = ℝ the following differential equation:
We can choose η(t) = 1, ϕ(t) = t. Then, it is easy to get that M(t) = (β + λ)/t, δ′(t) = 1/2, and therefore, from Theorem 6,
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
This research was supported by the National Natural Science Foundations of China (nos. 11171178, 61104136), the Natural Science Foundation of Shandong Province of China (no. ZR2010FQ002), and the Foundation of Qufu Normal University (no. XJ201014).