Nodal Solutions of the p-Laplacian with Sign-Changing Weight
Abstract
We are concerned with determining values of γ, for which there exist nodal solutions of the boundary value problem , u(0) = u(1) = 0, where m ∈ C[0,1] is a sign-changing function, f : ℝ → ℝ with f(s)s > 0. The proof of our main results is based upon global bifurcation techniques.
1. Introduction
-
H1 f ∈ C(ℝ, ℝ) with sf(s) > 0 for s ≠ 0;
-
m : [0,1]→[0, +∞) is continuous and does not vanish identically on any subinterval of [0,1];
-
there exist f0, f∞ ∈ (0, +∞) such that
()
Using the bifurcation theory of Rabinowitz [2, 3], they proved the following.
Theorem 1. Let (H1), (), and () hold. Assume that, for some k ∈ ℕ, either
The results of Theorem 1 have been extended to the case that the weight function changes its sign by Ma and Han [4]. Bifurcation methods have been applied to study the existence of nodal solutions of nonlinear two-point, multipoint, and periodic boundary value problems; see [5–9] and the references therein. The results they obtained extend some well-known theorems of the existence of positive solutions for the related problems [10].
However, no results on the existence of nodal solutions, even positive solutions, have been established for one-dimensional p-Laplacian equation with sign-changing weight m(t). It is the purpose of this paper to establish a similar result to Theorem 1 for one-dimensional p-Laplacian equation with sign-changing weight. Problem with sign-changing weight arises from the selection-migration model in population genetics. In this model, m(t) changes sign corresponding to the fact that an allele A1 holds an advantage over a rival allele A2 at the same points and is at a disadvantage at others; the parameter r corresponds to the reciprocal of diffusion; for details see [11].
If m(t) ≡ 1, Del Pino et al. [12] established the global bifurcation theory for one-dimensional p-Laplacian eigenvalue problem. Peral [13] got the global bifurcation theory for p-Laplacian eigenvalue problem on the unite ball. In [14], Del Pino and Manásevich obtained the global bifurcation from the principal eigenvalue for p-Laplacian eigenvalue problem on the general domain. If m(t) ≥ 0 and is singular at t = 0 or t = 1, Lee and Sim [15] also established the bifurcation theory for one-dimensional p-Laplacian eigenvalue problem. However, if m(t) changes sign, there are a few papers dealing with the p-Laplacian eigenvalue problem via bifurcation techniques. In [16], Drábek and Huang established the global bifurcation from the principal eigenvalue for p-Laplacian eigenvalue problem in ℝN.
-
H2 m(t) ∈ C[0,1] changes sign and
() -
H3 there exists f0 ∈ (0, ∞) such that
()
-
H4 there exists f∞ ∈ (0, +∞) such that
()
The main tool is the global bifurcation techniques in [17].
The rest of this paper is arranged as follows. In Section 2, we establish the global bifurcation theory for one-dimensional p-Laplacian eigenvalue problem with sign-changing weight. In Section 3, we state and prove the main results of this paper.
2. Some Preliminaries
Let Y = L1(0,1) with its usual normal .
The following spectrum result plays a fundamental role in our study.
Lemma 2 (see [18], [19].)Let (H2) hold. Then
- (i)
the set of all eigenvalues of the problem (13) is two infinite sequences of simple eigenvalues as follows:
() - (ii)
for k ∈ ℕ and ν ∈ {+, −}, Ker is a space of E with dimensional 1;
- (iii)
the eigenfunction corresponding to has exactly k − 1 simple zeros in (0,1).
Remark 3. Using the Gronwall inequality, we can easily show that all zeros of eigenfunction corresponding to eigenvalue are simple.
It is very known that is completely continuous in C1[0,1]. Thus, the Leray-Schauder degree is well-defined for arbitrary r-ball Br(0) and and ν ∈ {+, −}.
Lemma 4. For r > 0, we have
Proof. We divide the proof into two cases.
Case 1. λ ≥ 0. Since is compact and linear, by [20, Theorem 8.10] and Lemma 2 (ii) with p = 2,
If , then there are no such μ at all; then
If for some k ∈ ℕ, then
This together with Lemma 2 (ii) implies the following:
Case 2. λ < 0. In this case, we consider a new sign-changing eigenvalue problem as follows
We first show that the principle eigenvalue function is continuous.
Proposition 5. The eigenvalue function is continuous.
Proof. We only show that is continuous since the case of is similar. In the following proof, we will shorten to μ1. From the variational characterization of μ1(p), it follows that
Let be a sequence in (1, +∞) convergent to p > 1. We will show that
To do this, let . Then, from (24),
On applying the Dominated Convergence Theorem, we find that
Relation (27), the fact that u is arbitrary and (24) yield
Thus, to prove (25), it suffices to show that
Let us fix ɛ0 > 0 so that p − ɛ0 > 1 and, for each 0 < ɛ < ɛ0, is compactly embedded into Lp+ɛ(0,1). For k ∈ ℕ, let us choose such that
Thus,
Similarly, we can also obtain that
We note that (30) and (31) imply that
On the other hand, since uk⇀u in , from (32) we obtain that
Now, letting ɛ → 0+ and applying Fatou′s Lemma, we find that
Finally, combining (39) and (41), we obtain that
This and the variational characterization of μ1(p) imply (29) and hence (25). This concludes the proof of the lemma.
Using Remark 3, Lemma 2, and Proposition 5, we will show that all eigenvalue functions , 2 ≤ k ∈ ℕ are continuous.
Lemma 6. For fixed 2 ≤ k ∈ ℕ and ν ∈ {+, −}, as a function of p ∈ (1, +∞) is continuous.
Proof. Let be an eigenfunction corresponding to . By Lemma 2 and Remark 3, we know that u has exactly k − 1 simple zeros in I; that is, there exist ck,1, …, ck,k−1 ∈ I such that u(ck,1) = ⋯ = u(ck,k−1) = 0. For convenience, we set ck,0 = 0, ck,k = 1, and Ji = (ck,i−1, ck,i) for i = 1, …, k. Let denote the first positive or negative eigenvalue of the restriction of problem (13) on Ji for i = 1, …, k. Lemma 3 of [18] follows that for i = 1, …, k. Using a similar proof to Proposition 5, we can show that is continuous with respect to p for i = 1, …, k. Therefore, is also continuous with respect to p.
Lemma 7. (i) Let be the sequence of positive eigenvalues of (13). Let λ be a constant with for all k ∈ ℕ. Then, for arbitrary r > 0,
(ii) Let be the sequence of negative eigenvalues of (13). Consider , k ∈ ℕ; then
Proof. We will only prove the case since the proof for the other cases is similar. We also only give the proof for the case p > 2. Proof for the case 1 < p < 2 is similar. Assume that for some k ∈ ℕ. Since the eigenvalues depend continuously on p, there exists a continuous function χ : [2, p] → ℝ and q ∈ [2, p] such that and λ = χ(p). Define
It is easy to show that Φ(q, u) is a compact perturbation of the identity such that, for all u ≠ 0, by definition of χ(q), Φ(q, u) ≠ 0, for all q ∈ [2, p]. Hence, the invariance of the degree under homotopology and the classical result for p = 2 imply
For the existence of bifurcation branches for (12), we will make use of the following global bifurcation theorem results.
Lemma 8 (see [17].)Let X be a Banach space. Let F : ℝ × X → X be completely continuous such that F(λ, 0) = 0 for all λ ∈ ℝ. Suppose that there exist constants ρ, η ∈ ℝ, with ρ < η, such that (ρ, 0) and (η, 0) are not bifurcation points for the equation
- (i)
𝒞 is unbounded in ℝ × X or
- (ii)
𝒞∩[(ℝ∖[ρ, η]) × {0}] ≠ ∅.
Notice that (12) with λ = 0 has only the trivial solution. Applying this fact and Lemma 8 and the same method to prove [15, Theorem 2.1] with obvious changes, we may obtain the following.
Lemma 9. Assume that (H1), (H2), and (H3) hold. Then, for fixed p > 1 and for fixed σ ∈ {+, −}, each is a bifurcation point of (12) and the associated bifurcation branch satisfies the following;
- (1)
is unbounded in E;
- (2)
, where is the set of function which has exact k − 1 simple zeros in (0,1), and σu is positive near 0.
Lemma 10. Let (H2) hold. Let I = [a, b] be such that I ⊂ I+ and
Let gn : [0,1]→(0, +∞) be such that
Let yn ∈ E be a solution of the equation
Proof. After taking a subsequence if necessary, we may assume that
3. Main Results and Its Proof
Let be the kth positive or negative eigenvalue of (13). By applying Lemma 9, we will establish the main results as follows.
Theorem 11. Let (H1), (H2), (H3), and (H4) hold. Assume that, for some k ∈ ℕ, either
Then, (4) has two solutions and such that has exactly k − 1 zeros in (0,1) and is positive near 0 and has exactly k − 1 zeros in (0,1) and is negative near 0.
Proof. We only prove the case of γ > 0. The case of γ < 0 is similar. Consider the problem
Considering the results of Lemma 9, we have that, for each integer k ≥ 1, σ ∈ {+, −}, there exists a continuum of solutions of (62) joining to infinity in . Moreover, .
It is clear that any solution of (62) of the form (1, u) yields a solution u of (4). We will show that crosses the hyperplane {1} × E in ℝ × E. To this end, it will be enough to show that joins to . Let satisfy
Case 1. . In this case, we only need to show that
Step 1. We show that, if there exists a constant number M > 0 such that
In this case, it follows that
Let ξ ∈ C(ℝ) be such that
We divide the equation
By the continuity and compactness of Gp, it follows that
We claim that
Suppose on the contrary that . Since is a solution of (74) and all zeros of in [0,1] are simple, it follows that for some h ∈ ℕ and ι ∈ {+, −}.
By the openness of , we have that there exists a neighborhood such that
Step 2. We show that there exists a constant M such that μn ∈ (0, M] for n ∈ ℕ large enough.
On the contrary, we suppose that
Since , it follows that
Let
However, this contradicts (H2): 0 < meas I− < 1.
Case 2. . In this case, we have that
Assume that is such that
If ηn → +∞, then we are done!
If there exists M > 0, such that, for n ∈ ℕ sufficiently large,
Applying the same method used in Step 1 of Case 1, after taking a subsequence and relabeling if necessary, it follows that
Thus, joins to .
Acknowledgments
This paper was supported by the NSFC (nos. 11061030, 11361047, and 11201378), SRFDP (no. 20126203110004), and Gansu Provincial National Science Foundation of China (no. 1208RJZA258).