Volume 2013, Issue 1 406350
Research Article
Open Access

Nodal Solutions of the p-Laplacian with Sign-Changing Weight

Ruyun Ma

Corresponding Author

Ruyun Ma

Department of Mathematics, Northwest Normal University, Lanzhou 730070, China nwnu.edu.cn

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Xilan Liu

Xilan Liu

Department of Mathematics, Qinghai University for Nationalities, Xining 810007, China qhu.edu.cn

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Jia Xu

Jia Xu

Department of Mathematics, Northwest Normal University, Lanzhou 730070, China nwnu.edu.cn

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First published: 27 November 2013
Citations: 1
Academic Editor: Paul Eloe

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 mC[0,1] is a sign-changing function, f : with f(s)s > 0. The proof of our main results is based upon global bifurcation techniques.

1. Introduction

In [1], Ma and Thompson considered determining values of r, for which there exist nodal solutions of the boundary value problem
()
under the following assumptions:
  • H1 fC(, ) 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, either

()
Then (1) 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.

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 [59] 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 N.

The purpose of this paper is to study the bifurcation behavior of one-dimensional p-Laplacian eigenvalue problem as follows:
()
under the condition (H1) and
  • H2 m(t) ∈ C[0,1] changes sign and

    ()

  • H3 there exists f0 ∈ (0, ) such that

    ()

where φp(s) = |s|p−2s with 1 < p < +;
  • H4 there exists f ∈ (0, +) such that

    ()

Moreover, based on our global bifurcation theorem, we will prove the existence of nodal solutions for the corresponding nonlinear problem with a parameter (see Theorem 11).

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 E be the Banach space with the norm
()

Let Y = L1(0,1) with its usual normal .

We start by considering the following auxiliary problem:
()
for a given hL1(0,1). By a solution of problem (9), we understand a function uE with φp(u) absolutely continuous which satisfies (9). Problem (9) is equivalently written to
()
where a : Y is a continuous function satisfying
()
It is known that Gp : YE is continuous and maps equi-integrable sets of Y into relatively compacts of E. One may refer to Lee and Sim [15] for details.
Since the bifurcation points of
()
is related to the eigenvalues of the problem
()
We define the operator by
()
Then is completely continuous and problem (13) is equivalent to
()

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 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,

()
where m(λ) is the sum of algebraic multiplicity of the eigenvalues μ of (13) satisfying μ−1λ > 1.

If , then there are no such μ at all; then

()

If for some k, 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

()
where λ = −λ, . It is easy to check that
()
Thus, we may use the result obtained in Case 1 to deduce the desired result.

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 be a subsequence of such that .

Let us fix ɛ0 > 0 so that pɛ0 > 1 and, for each 0 < ɛ < ɛ0, is compactly embedded into Lp+ɛ(0,1). For k, let us choose such that

()
()
For 0 < ɛ < ɛ0, there exists k0 such that pɛ < pk < p + ɛ for any kk0. Thus, for kk0, (30) and Hölder′s inequality imply that
()
This shows that is a bounded sequence in . Passing to a subsequence if necessary, we can assume that uku in and hence that uku in Lp+ɛ(0,1). Furthermore, uLp(0,1) and uku in for kk0. It follows that
()
as k → +. It is clear that
()

Thus,

()

Similarly, we can also obtain that

()
where m+(t) = max {m(t), 0} and m(t) = −min {m(t), 0}. Therefore,
()

We note that (30) and (31) imply that

()
for all k. Thus, letting k go to + in (38) and using (37), we find that
()

On the other hand, since uku in , from (32) we obtain that

()

Now, letting ɛ → 0+ and applying Fatou′s Lemma, we find that

()
Hence, uW1,p(0,1); here W1,p(0,1) denotes the radially symmetric subspace of W1,p(0,1). We claim that actually . Indeed, we know that for each 0 < ɛ < ɛ0. For , it is easy to see that
()
Then, letting ɛ → 0+, we obtain that
()
where p = p/(p − 1). Since ϕ is arbitrary, from Proposition IX-18 of [21], we find that , as desired.

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 are continuous.

Lemma 6. For fixed 2 ≤ k 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−1I 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. Then, for arbitrary r > 0,

()
where β is the number of eigenvalues of problem (13) less than λ.

(ii) Let be the sequence of negative eigenvalues of (13). Consider , k; then

()
where β is the number of eigenvalues of problem (25) larger than λ.

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. Since the eigenvalues depend continuously on p, there exists a continuous function χ : [2, p] → 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 : × XX be completely continuous such that F(λ, 0) = 0 for all λ. Suppose that there exist constants ρ, η, with ρ < η, such that (ρ, 0) and (η, 0) are not bifurcation points for the equation

()
Furthermore, assume that
()
where Br(0) = {uX : ∥u∥ < r} is an isolating neighborhood of the trivial solution for both constants ρ and η. Let
()
and let 𝒞 be the component of 𝒮 containing [ρ, η]×{0}. Then, either
  • (i)

    𝒞 is unbounded in × X or

  • (ii)

    𝒞∩[(∖[ρ, η]) × {0}] ≠ .

Define the Nemytskii operators H : × EY by
()
Then, it is clear that H is continuous operator which sends bounded sets of × E into an equi-integrable sets of Y and problem (12) can be equivalently written as
()
F is completely continuous in × EE and F(λ, 0) = 0, for all λ.

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.

Finally, we give a key lemma that will be used in Section 3. Let
()

Lemma 10. Let (H2) hold. Let I = [a, b] be such that II+ and

()

Let gn : [0,1]→(0, +) be such that

()

Let ynE be a solution of the equation

()
Then, the number of zeros of yn|I goes to infinity as n → +.

Proof. After taking a subsequence if necessary, we may assume that

()
as j → +. It is easy to check that the distance between any two consecutive zeros of any nontrivial solution of the equation
()
goes to zero as j → +. Using this with [21, Lemma 2.5], it follows the desired results.

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, either

()
or
()

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 × E. To this end, it will be enough to show that joins to . Let satisfy

()
We note that ηn > 0 for all n since (0,0) is the only solution of (62) for λ = 0 and .

Case  1. . In this case, we only need to show that

()
We divide the proof into two steps.

Step  1. We show that, if there exists a constant number M > 0 such that

()
for n large enough, then joins to .

In this case, it follows that

()

Let ξC() be such that

()
Then,
()
Let
()
Then, is nondecreasing and
()

We divide the equation

()
by ∥yn∥ and set . Since is bounded in E, after taking a subsequence if necessary, we have for some and in Y with . Moreover, from (70) and the fact that is nondecreasing, we have
()
since
()

By the continuity and compactness of Gp, it follows that

()
where , again choosing a subsequence and relabeling if necessary.

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 and ι ∈ {+, −}.

By the openness of , we have that there exists a neighborhood such that

()
which contradicts the facts that in E and . Therefore, . Moreover, by Lemma 2, , so that
()
Therefore, joins   to .

Step  2. We show that there exists a constant M such that μn ∈ (0, M] for n large enough.

On the contrary, we suppose that

()

Since , it follows that

()

Let

()
be the zeros of yn in [0,1]. Then, after taking a subsequence if necessary,
()
Notice that Lemma 10 and the fact that yn has exactly k − 1 simple zeros in [0,1] yield
()
which implies that
()

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 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).

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