The Existence of Positive Solutions for a Nonlinear Sixth-Order Boundary Value Problem
Abstract
By using the Krein-Rutman theorem and bifurcation methods, we discuss the existence of positive solutions for the boundary value problems of a sixth-order ordinary differential equation.
1. Introduction
In [2], the existence and multiplicity results of nontrivial solutions for (1.1) were proved using a minimization theorem and Clarks theorem [6], respectively, when C = 1 and f(x, u) = u3. The authors studied also the homoclinic solutions for (1.1) when C = −1 and f(x, u) = −a(x)u | u|σ, where a(x) is a positive periodic function and σ is a positive constant, by the mountain-pass theorem and concentration-compactness arguments. In [3], by variational tools, including Brezis-Nirenbergs linking theorems, Gyulov et al. studied also the existence and multiplicity of nontrivial solutions of BVP (1.1). In [7], using the fixed point index theory of cone mapping, the authors gave some results for existence and multiplicity of positive solutions of BVP (1.1).
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A1 f : [0,1]×[0, ∞)×(−∞, 0]×[0, ∞)→[0, ∞) is continuous and there exist functions a, b, c, d, m, n ∈ C([0,1, 0, ∞)) with a(t) + b(t) + c(t) > 0 and d(t) + m(t) + n(t) > 0 on [0,1] such that
(1.5)uniformly for t ∈ [0,1], and(1.6)uniformly for t ∈ [0,1]. Here . -
A2 f(t, u, p, q) > 0 for t ∈ [0,1] and (u, p, q)∈([0, ∞)×(−∞, 0]×[0, ∞))∖{(0,0, 0)}.
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A3 There exist constants a0, b0, c0 ∈ [0, ∞) satisfying and f(t, u, p, q) ≥ a0u − b0p + c0q + o(|(u, p, q)|) for (t, u, p, q)∈[0,1]×[0, ∞)×(−∞, 0]×[0, ∞).
The existence of positive solution for (1.4) is proved using Krein-Rutman theorem [10] and the Global Bifurcation Theory [11]. The idea of this work comes from [8, 9].
The rest of the paper is organized as follows. In Section 2, we present some preliminaries and lemmas that will be used to prove our main results. In Section 3, we discuss the existence of positive solution of the problem (1.4).
2. Preliminaries
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A4 A, B, C ∈ C([0,1], [0, ∞)) with A(t) > 0 or B(t) > 0 or C(t) > 0 with t ∈ [0,1].
Definition 2.1. We say μ is a generalized eigenvalue of the linear problem
Lemma 2.2. For u ∈ X, then ∥u∥∞ ≤ ∥u′∥∞ ≤ ∥u′′∥∞ ≤ ∥u′′′∥∞ ≤ ∥u(4)∥∞ ≤ ∥u∥X.
Proof. (1) By u(0) = u(1), there is a ξ ∈ (0,1) such that u′(ξ) = 0, and so . Hence . By u′′(0) = u′′(1), there is a η ∈ (0,1), which makes u′′′(η) = 0, thereby we come to . And we have .
(2) Because of u(0) = 0, we come to . Correspondingly, ∥u∥∞ ≤ ∥u′∥∞ and we can obtain ∥u′′∥∞ ≤ ∥u′′′∥∞ for the same reason.
(3) By the definition of X, we know |u(4)(t)| ≤ ɛe(t) ≤ ɛ, that is, |u(4)|∞ ≤ ɛ. Correspondingly, we come to |u(4)|∞≤|u|X.
Based on the combination of (1), (2) and (3), the conclusion can be reached and the lemma is thus proved.
Theorem 2.3. Assume that (A4) holds, let r(t) be the spectral radius of T, then Problem (2.1) has an algebraically simple eigenvalue, μ1(A, B, C) = (r(t)) −1, with a positive eigenfunction . Moreover, there is no other eigenvalue with a positive eigenfunction.
Proof. It is easy to check that Problem (2.1) is equivalent to the integral equation u(t) = μTu(t).
We define T : X → X.
In fact, for u ∈ X, we have
If u ∈ P, then [A(s)u(s) − B(s)u′′(s) + C(s)u(4)(s)] ≥ 0, s ∈ [0,1], and correspondingly,
Because T(X) ⊂ C6[0,1]∩X, and C6[0,1]∩X is compactly embedded in X, thus we obtain that T : X → X is completely continuous.
Next, we will prove that T : X → X is strongly positive.
(1) For any u ∈ P∖{0}, if A(t) > 0 on [0,1], then there exists a constant k > 0 such that
For any u ∈ P∖{0}, if B(t) > 0 on [0,1], then there exists a constant k1 > 0 such that
For any u ∈ P∖{0}, if C(t) > 0 on [0,1], similarly, we can verify that there exists r3 > 0, which makes Tu(t) ≥ r3e(t) on [0,1].
Hence we obtain Tu(t) ≥ re(t), for all t ∈ [0,1], in which r = min {r1, r2, r3}.
(2) Thanks to the definition of T, we come to
(3) It is easy to come to
By (1), (2), and (3), we have .
According to Krein-Rutman theorem, we know that T has a single algebraic eigenvalue r(T) > 0 which corresponds to the eigenvector . Furthermore, there is no other eigenvalues with corresponding positive eigenfunctions. Correspondingly, μ1(A, B, C) = (r(t)) −1 is an algebraic single eigenvalue of Problem (2.1) with a corresponding positive eigenvector , and there is no any other eigenvalues which have corresponding positive feature vector. The theorem is thus proved.
3. Main Results
The main result of this paper is as follows.
Theorem 3.1. Let (A1), (A2), and (A3) hold. Assume that either
Proof. Define that L : D(L) → Y by L(u): = −u(6), u ∈ D(L), where
Let ζ, ξ ∈ C([0,1]×[0, ∞)×(−∞, 0]×[0, ∞)), and satisfy
Let us consider
It is easy to verify that (3.7) is equivalent to equation
There exists an unbounded connected subset Γ for the following set:
Next, we will verify the result of this theorem.
Obviously, any solution of (3.7), such as (1, u), is the solution of problem (1.4). If we want to verify Γ passing through hyperplane {1} × X, we only need to verify that Γ connects (μ1(a, b, c), 0) and (μ1(d, m, n), ∞).
Let (ηn, yn) ∈ Γ and satisfy
Case 1 (μ1(d, m, n) < 1 < μ1(a, b, c)). If we want to verify that (1.4) have at least one positive solution, we only need to verify that Γ connects (μ1(a, b, c), 0) and (μ1(d, m, n), ∞), that is, to verify
Step 1. If we can verify that there exists a constant M > 0 such that ηn ⊂ [0, M], where n ∈ N, then this connects (μ1(a, b, c), 0) and (μ1(d, m, n), ∞).
By (3.13), when n → ∞, ∥yn∥X → ∞, and we divide the two sides of equation
Step 2. To verify the fact that arbitrary n ∈ N, there exists m > 0 such that ηn ⊂ [0, M].
Thanks to the Lemma 2.1 in [8], we only need to verify that nonlinear operator R(λ, u) has linear function V, and there exists (η, y)∈(0, ∞) × P such that ∥y∥X = 1 and ηVy ≥ y. It follows from (A3) that there exist a0, b0, c0 ∈ [0, ∞) such that , and
Again, as
Case 2 (μ1(a, b, c) < 1 < μ1(d, m, n)). If (ηn, yn) ∈ Γ, which satisfies lim n→∞ηn + ∥yn∥X = ∞, and lim n→∞∥yn∥X = ∞, then we obtain
Similar to Case 1, the verification of Case 2 can also be divided into two steps with the conclusion that Γ connects (μ1(a, b, c), 0) and (μ1(d, m, n), ∞). And we come to the conclusion that Γ passes through hyperplane {1} × X on R × X, hence (1.4) have at least one positive solution.
Acknowledgments
The author are very grateful to the anonymous referees for their valuable suggestions and to be sponsored by the Tutorial Scientific Research Program Foundation of Education Department of Gansu Province China (1110-05).