Positive Periodic Solution for Second-Order Singular Semipositone Differential Equations
Abstract
We study the existence of a positive periodic solution for second-order singular semipositone differential equation by a nonlinear alternative principle of Leray-Schauder. Truncation plays an important role in the analysis of the uniform positive lower bound for all the solutions of the equation. Recent results in the literature (Chu et al., 2010) are generalized.
1. Introduction
During the last two decades, the study of the existence of periodic solutions for singular differential equations has attracted the attention of many researchers [1–4]. Some strong force conditions introduced by Gordon [5] are standard in the related earlier works [6, 7]. Compared with the case of a strong singularity, the study of the existence of periodic solutions under the presence of a weak singularity is more recent [2, 8, 9], but has also attracted many researchers. Some classical tools have been used to study singular differential equations in the literature, including the method of upper and lower solutions [10], degree theory [11], some fixed point theorem in cones for completely continuous operators [12], Schauder’s fixed point theorem [8, 9, 13], and a nonlinear Leray-Schauder alternative principle [2, 3, 14, 15].
However the singular differential equations, in which there is the damping term, that is, the nonlinearity is dependent on the derivative, has not attracted much attention in the literature. Several existence results can be found in [14, 16, 17].
The aim of this paper is to further show that the nonlinear Leray-Schauder alternative principle can be applied to (1) in the semipositone cases, that is, f(t, x, x′)≥−M for some M > 0.
In this paper, let us fix some notations to be used in the following: given φ ∈ L1[0, T], we write φ≻0 if φ ≥ 0 for almost everywhere t ∈ [0, T] and it is positive in a set of positive measure. The usual Lp-norm is denoted by ∥·∥p. p* and p* the essential supremum and infinum of a given function p ∈ L1[0, T], if they exist.
2. Preliminaries
In other words, the strict antimaximum principle holds for (4)-(5).
Definition 1. We say that (4) admits the antimaximum principle if (6) has a unique T-periodic solution for any l ∈ ℂ(ℝ/Tℤ) and the unique T-periodic solution xl(t) > 0 for all t if l≻0.
Lemma 2 (see [14], Corollary 2.6.)Assume that a≢0 and the following two inequalities are satisfied:
Next, recall a well-known nonlinear alternative principle of Leray-Schauder, which can be found in [20] and has been used by Meehan and O’Regan in [4].
Lemma 3. Assume Ω is an open subset of a convex set K in a normed linear space X and p ∈ Ω. Let be a compact and continuous map. Then one of the following two conclusions holds:
- (I)
T has at least one fixed point in .
- (II)
There exists x ∈ ∂Ω and 0 < λ < 1 such that x = λTx + (1 − λ)p.
In applications below, we take with the norm ∥x∥ = max t∈[0,T] | x(t)| and define .
3. Main Results
In this section, we prove a new existence result of (1).
Theorem 4. Suppose that (4) satisfies (A) and
- (H1)
F(t, x, y) = f(t, x, y) + M ≥ 0 for all (t, x, y)∈[0, T]×(0, r] × R.
- (H2)
f(t, x, y) ≥ g0(x) for (t, x, y)∈[0, T]×(0, R0] × R, where the nonincreasing continuous function g0(x) > 0 satisfies and .
- (H3)
0 ≤ F(t, x, y)≤(g(x) + h(x))ϱ(|y|), for all (t, x, y)∈[0, T]×(0, r] × R, where g(·) > 0 is nonincreasing in (0, r] and h(·)/g(·) ≥ 0, ϱ(·) ≥ 0 are nondecreasing in (0, r].
- (H4)
()
-
where
() -
Then (1) has at least one positive periodic solution u(t) with 0 < ∥u + Mw∥≤r.
Proof. For convinence, let us write Z(t) = x(t) − Mw(t), Zn(t) = xn(t) − Mw(t), where w(t) = (ℒ1)(t). Let
Choose n0 ∈ {1,2, …} such that 1/n0 < r, and then let N0 = {n0, n0 + 1 + ⋯}.
Consider the family of equations
A T-periodic solution of (17) is just a fixed of the operator equation
We claim that for any T-periodic solution xn(t) of (17) satisfies
By the periodic boundary conditions, we have x′(t0) = 0 for some t0 ∈ [0, T]. Therefore,
Choose n1 ∈ N0 such that 1/n1 ≤ R1, and then let N1 = {n1, n1 + 1, …}. The following lemma holds.
Lemma 5. There exists an integer n2 > n1 large enough such that, for all n ∈ N2 = {n2, n2 + 1, …},
Proof. The lower bound in (27) is established by using the strong force condition of f(t, x, y). By condition (H2), there exists R1 ∈ (0, R0) and a continuous function such that
For n ∈ N1, let αn = min 0≤t≤TZn(t), βn = max 0≤t≤TZn(t).
If αn ≥ R1, due to n ∈ N1, (27) holds.
If αn < R1, we claim that, for all n ∈ N1,
Due to αn < R1, that is, αn = min 0≤t≤T[xn(t) − Mw(t)] = xn(an) − Mw(an) < R1 for some an ∈ [0, T]. By (29), there exists cn ∈ [0, T] (without loss of generality, we assume an < cn.) such that xn(cn) = Mw(cn) + R1 and xn(t) ≤ Mw(t) + R1 for an ≤ t ≤ cn.
It can be checked that
In fact, if t ∈ [an, cn] is such that 1/n ≤ Zn(t) ≤ R1, we have
Using (17) (with λ = 1) for xn(t) and the estimation (34), we have, for t ∈ [an, cn]
Suppose that (27) does not hold, that is, for some n ∈ N1, Zn(t) < 1/n < R1. Then there would exist bn ∈ (an, cn) such that Zn(bn) = 1/n and
By the facts ∥xn∥ < r, , ∥w′∥ ≤ r and the definition of Zn(t), we can obtain , together with ∥xn∥<r, implies that the second term and the third term are bounded. The first term is
Furthermore, we can prove Zn(t) has a uniform positive lower bound δ.
Lemma 6. There exist a constant δ > 0 such that, for all n ∈ N2,
Proof. Multiplying (17) (with λ = 1) by and integrating from an to cn, we obtain
In the same way as in the proof of (41), one way readily prove that the right-hand side of the above equality is bounded. On the other hand, if n ∈ N2, by (H2),
Next, we will prove (17) has periodic solution xn(t).
For ιr > 0, we can choose n3 ∈ N2 such that 1/n3 < ιr, which together with (H4) imply
Next we claim that any fixed point xn of (18) for any λ ∈ [0,1] must satisfy ∥xn∥≠r. So, by using the Leray-Schauder alternative principle, (17) (with λ = 1) has a periodic solution xn(t). Otherwise, assume that xn is a fixed point xn of (18) for some λ ∈ [0,1] such that ∥xn∥ = r. Note that
The fact ∥xn∥<r and show that is a bounded and equicontinuous family on [0, T]. Now Arzela-Ascoli Theorem guarantees that has a subsequence , converging uniformly on [0, T] to a function x ∈ C [0, T]. From the fact ∥xn∥<r and xn(t) > δ, x satisfies δ ≤ x(t) ≤ r for all t. Moreover, satisfies the integral equation
Corollary 7. Let the nonlinearity in (1) be
Proof. We will apply Theorem 4 with M = max 0≤t≤T | e(t)| and g(x) = x−α, h(x) = μxβ + 2M, ϱ(y) = 1+|y|γ. Then condition (H1)–(H3) are satisfied and existence condition (H4) becomes
Acknowledgments
The research of X. Xing is supported by the Fund of the Key Disciplines in the General Colleges and Universities of Xin Jiang Uygur Autonomous Region (Grant no. 2012ZDKK13). It is a pleasure for the author to thank Professor J. Chu for his encouragement and helpful suggestions.