Startseite Positive Answer to Berestycki’s Open Problem on the Unit Ball
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Positive Answer to Berestycki’s Open Problem on the Unit Ball

  • Guowei Dai EMAIL logo und Bianxia Yang
Veröffentlicht/Copyright: 2. September 2016

Abstract

In this paper, we establish a unilateral global bifurcation result from intervals for a class of semilinear problems on the unit ball. By applying the above result, we obtain the spectrum of a class of half-linear problems on the unit ball. Our results partially give a positive answer to the open problem proposed by Berestycki.

MSC 2010: 34C23; 35P30

1 Introduction

In [3], Berestycki proposed an open problem: does the equation

{ - Δ u = λ u + | u | in Ω , u = 0 on Ω

possess infinitely many half-eigenvalues? The aim of this paper is to give a positive answer to this open problem on the unit ball. To do this, we first study global bifurcation phenomena for the following problem on the unit ball:

(1.1) { - Δ u = λ u + F ( x , u , λ ) in B , u = 0 on B ,

where B is the unit open ball of N with N1, λ is a parameter, and F:B¯×2 is a continuous function and radially symmetric with respect to x.

It is clear that the radial solution of (1.1) is equivalent to the solution of the following problem:

(1.2) { - ( r N - 1 u ) = λ r N - 1 u + r N - 1 F ( r , u , λ ) , r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 ,

where r=|x| with xB. We also assume that the nonlinear term F has the form F=f+g, where f and g satisfy the following conditions:

  1. |f(r,s,λ)|M|s| for all r[0,1], 0<|s|1 and λ, where M is a positive constant;

  2. g(r,s,λ)=o(|s|) near s=0, uniformly in r[0,1] and on bounded λ intervals.

Let E={uC1[0,1]:u(0)=u(1)=0} be the space endowed with the norm

u = max r [ 0 , 1 ] | u ( r ) | + max r [ 0 , 1 ] | u ( r ) | .

Let Sk+ denote the set of functions in E which have exactly k-1 interior nodal zeros in (0,1) and u(0)>0, and set Sk-=-Sk+ and Sk=Sk+Sk-. It is clear that Sk+ and Sk- are disjoint and open in E. Also, let Φk±=×Sk± and Φk=×Sk under the product topology. We use 𝒮 to denote the closure of the nontrivial solutions set of problem (1.2) in ×E, and 𝒮k± to denote the subset of 𝒮 with uSk± and 𝒮k=𝒮k+𝒮k-. Finally, let λk be the kth eigenvalue of the following eigenvalue problem:

{ - ( r N - 1 u ) = λ r N - 1 u , r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 .

It is well known that λk is positive and simple, and the eigenfunction corresponding to it has exactly k-1 simple zeros in (0,1). The unilateral global bifurcation result for problem (1.2) is the following theorem.

Theorem 1

Let Ik=[λk-M,λk+M] for every kN. The component Ck+ of Sk+(Ik×{0}), containing Ik×{0}, is unbounded and lies in Φk+(Ik×{0}) and the component Ck- of Sk-(Ik×{0}), containing Ik×{0}, is unbounded and lies in Φk-(Ik×{0}).

Theorem 1 is a generalization of [8, Theorem 4.1] (in the case of p=2) given by Del Pino and Manasevich. After that there has been some progress in this topic, for example, see [10, 12, 14] and the references therein. In these mentioned papers, the nonlinearities are Fréchet differentiable or (p-1)-homogeneous linearizable at the origin. However, the nonlinear term of problem (1.2) is not necessary linearizable at the origin because of the influence of the term f. Problems with nondifferentiable nonlinearities have been studied by many mathematicians. In [3], Berestycki considered a class of Sturm–Liouville problems with nondifferentiable nonlinearities. Berestycki’s results have been improved partially by Schmitt and Smith [17] by applying a set-valued version of Rabinowitz’s global bifurcation theorem. These results have been extended by Rynne [16] (with the help of some estimates coming from [2]) under some suitable assumptions.

We shall use the unilateral global bifurcation theorem of [5] rather than the global bifurcation theorem of [15] which was used by Berestycki in [3]. We refer to [5, 7, 13, 15, 18] and their references for the theory of unilateral global bifurcation. Based on the unilateral global interval bifurcation result, we establish the spectrum of the following problem:

(1.3) { - ( r N - 1 u ) = λ r N - 1 u + α ( r ) r N - 1 u + + β ( r ) r N - 1 u - , r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 ,

where u+=max{u,0}, u-=-min{u,0}, α and β are two continuous functions defined on [0,1]. Problem (1.3) is called half-linear because it is positively homogeneous and linear in the cones u>0 and u<0. Similar to [3], we say that λ is a half-eigenvalue of problem (1.3) if there exists a nontrivial solution (λ,uλ). The eigenvalue λ is said to be simple if v=cuλ, c>0, for all solutions (λ,v) of problem (1.3). More precise, we shall use Theorem 1 to prove the following result.

Theorem 2

There exist two sequences λ1+<λ2+<<λk+< and λ1-<λ2-<<λk-< of simple half-eigenvalues for problem (1.3). The corresponding half-linear solutions are in {λk+}×Sk+ and {λk-}×Sk-. Furthermore, aside from these solutions and the trivial one, there is no other solution of problem (1.3).

Theorem 2 shows that problem (1.3) does possess two sequences of simple half-eigenvalues, which gives a positive answer to the open problem proposed by Berestycki. Moreover, the conclusions of Theorem 2 are related to the radial Fučik spectrum of the following problem:

{ - ( r N - 1 u ) = a r N - 1 u + - b r N - 1 u - , r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 ,

which was obtained by Arias and Campos [1]. To explain this, let α(r)β(r)=1, λ+1=a and 1-λ=b. Then (λk±+1,1-λk±), k, are just the Fučik spectrum point. In this sense, in the case α(r)β(r)=1, problem (1.3) is a particular case of the study by Arias and Campos. The Fučik spectrum was introduced by Fučik [11] and Dancer [6] in the study of semilinear elliptic problems with jumping nonlinearities. For ordinary differential equations of second-order, Fučik [11] gave a complete description of this spectrum. Later on, Drábek [9] characterized the spectrum for the one-dimensional p-Laplacian, which has similar properties to that of the linear ODE case.

Let φiν denote the eigenfunction corresponding to λiν with φiν=1, ν{+,-}, i. Let, in addition, 0<τ1<<τk=1 denote the zeros of φiν. If β(r)-α(r) in (0,1)Zk, where Zk={τ1,,τk-1}, then clearly λk+=λk- (see Remark 7). In particular, if β(r)-α(r)0 in (0,1)Zk, then we have that λk+=λk-=λk. Otherwise, we have the following corollary.

Corollary 3

If β(r)-α(r) in (0,1)Zi, then λi+λi- for any iN.

Moreover, we also have the following corollary.

Corollary 4

For any i, jN, if ij, then λj-λi+.

The above two corollaries show that both sequences obtained in Theorem 2 cannot coincide under the assumption of β(r)-α(r) in (0,1)Zi for any i, that is to say, λi+λj- for any i,j. In particular, both sequences cannot coincide if β(r)-α(r) for any r(0,1).

The rest of this paper is arranged as follows. In Section 2, we give the proof of Theorem 1. In Section 3, we prove Theorem 2, and Corollaries 3 and 4.

2 Proof of Theorem 1

First, we have the following existence and uniqueness result for problem (1.2).

Lemma 5

If (λ,u) is a solution of problem (1.2) under the assumptions (C1) and (C2) and u has a double zero, then u0.

Proof.

Let u be a solution of (1.2) and r*[0,1] be a double zero. We note that

u ( r ) = - r * r ( λ u + F ( τ , u , λ ) ) ( τ r ) N - 1 𝑑 τ .

If r*=0, then we have that

| u ( r ) | 0 r | ( λ u + F ( τ , u , λ ) ) | ( τ r ) N - 1 𝑑 τ r N sup τ [ 0 , r ] ψ ( τ ) ,

where ψ(r)=|λu(r)+F(r,u(r),λ)|. In view of (C1) and (C2), for any ε>0, there exists a constant δ>0 such that

| F ( r , s , λ ) | ( ε + M ) | s |

uniformly with respect to r[0,1] and fixed λ when |s|[0,δ]. Hence,

| u ( r ) | r N 0 r K λ | u ( τ ) | 𝑑 τ ,

where

K λ = | λ | + ε + M + max τ [ 0 , 1 ] max s [ δ , u ] | F ( τ , s , λ ) s | .

By the Gronwall–Bellman inequality [4], we get u(r)0 on [0,1]. It follows that u(r)0 on [0,1].

Next, we assume that r*>0. First, we consider r[0,r*]. Note that

u ( r ) = - r * r r * s ( λ u + F ( τ , u , λ ) ) ( τ s ) N - 1 𝑑 τ 𝑑 s .

Then

r N - 1 | u ( r ) | r r * K λ τ N - 1 | u ( τ ) | 𝑑 τ .

From the Gronwall–Bellman inequality, it follows that rN-1|u(r)|0 on [0,r*]. Therefore, u0 on (0,r*]. Furthermore, the continuity of u shows that u0 on [0,r*]. Now, for the case of r[r*,1], we have that

( r * ) N - 1 | u ( r ) | r * r K λ τ N - 1 | u ( τ ) | 𝑑 τ r * r K λ | u ( τ ) | 𝑑 τ .

Again by the Gronwall–Bellman inequality, we get u0 on [r*,1]. ∎

To prove Theorem 1, we introduce the following approximate problem:

(2.1) { ( r N - 1 u ) + λ r N - 1 u + r N - 1 f ( r , u | u | ε , λ ) + r N - 1 g ( r , u , λ ) = 0 , r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 .

The next lemma ensures that (𝒮kν(×{0}))(Ik×{0}) and plays a key role in this paper.

Lemma 6

Let ϵn, 0ϵn1, be a sequence converging to 0. If there exists a sequence (λn,un)(R×Skν) such that (λn,un) is a nontrivial solution of problem (2.1) corresponding to ϵ=ϵn, and (λn,un) converges to (λ,0) in R×E, then λIk.

Proof.

Let wn=un/un, then wn should be a solution of the following problem:

(2.2) { - ( r N - 1 w n ) = λ n r N - 1 w n + r N - 1 f ( r , u n | u n | ε n , λ n ) u n + r N - 1 g ( r , u n , λ n ) u n , r ( 0 , 1 ) , w n ( 0 ) = w n ( 1 ) = 0 .

Let

g ~ ( r , u , λ ) = max 0 | s | u | g ( r , s , λ ) |

for all r[0,1] and λ on bounded sets. Then g~ is nondecreasing with respect to u and

(2.3) lim u 0 + g ~ ( r , u , λ ) u = 0 .

Further, from (2.3), it follows that

(2.4) | g ( r , u , λ ) u | g ~ ( r , | u | , λ ) u g ~ ( r , u , λ ) u g ~ ( r , u , λ ) u 0 as u 0

uniformly in r[0,1] and λ on bounded sets. Clearly, (C1) implies that

(2.5) | f ( r , u n | u n | ϵ n , λ n ) u n | = | f ( r , u n | u n | ϵ n , λ n ) u n | u n | ϵ n u n | u n | ϵ n u n | M u n ϵ n M as n +

for all r[0,1]. It is obvious that (2.2), (2.4) and (2.5) imply that vn:=rN-1wn is bounded in C1. Therefore, by the Arzelà–Ascoli theorem, we may assume that vnv in C0. It follows that wnv~ in C0. Obviously,

w n ( r ) = 1 r w n ( τ ) 𝑑 τ 1 r v ~ ( τ ) 𝑑 τ in C 0 .

Hence, wn is strong convergent in C1. Without loss of generality, we may assume that wnw in C1, w=1. Clearly, we have that wSkν¯.

We claim that wSkν. On the contrary, we suppose that wSkν. Then w has at least one double zero r*[0,1]. It follows that wn(r*)0 and wn(r*)0 as n+. We note that

r N - 1 w n ( r ) = r * r τ N - 1 ( - λ n w n - f ( τ , u n | u n | ε n , λ n ) u n - g ( τ , u n , λ n ) u n ) 𝑑 τ + ( r * ) N - 1 w n ( r * ) .

If r*=0, we have that

r N - 1 w n ( r ) = 0 r τ N - 1 ( - λ n w n - f ( τ , u n | u n | ε n , λ n ) u n - g ( τ , u n , λ n ) u n ) 𝑑 τ .

It follows that

r N - 1 | w n ( r ) | 0 r τ N - 1 | λ n w n + f ( τ , u n | u n | ε n , λ n ) u n + g ( τ , u n , λ n ) u n | 0 r W ( τ , u n , λ n , w n , ε n ) τ N - 1 | w n | 𝑑 τ ,

where

W = | λ n | + | f ( τ , u n | u n | ε n , λ n ) u n w n | + | g ( τ , u n , λ n ) u n w n | .

In view of (C2) and the definition of wn, we can show that

| g ( r , u n , λ n ) u n w n | = | g ( r , u n , λ n ) u n | 0 as n +

uniformly in r[0,1]. Similarly, (C1) implies that

| f ( r , u n | u n | ε n , λ n ) u n w n | = | f ( r , u n | u n | ε n , λ n ) u n | u n | ϵ n | | u n | ϵ n M | u n | ϵ n M as n +

for all r[0,1]. Hence, there exists a positive constant K such that

( | λ n | + | f ( r , u n | u n | ε n , λ n ) u n w n | + | g ( r , u n , λ n ) u n w n | ) K

for all r[0,1] and n large enough. Clearly, one has that

w n ( r ) = 0 r w n ( τ ) 𝑑 τ + w n ( 0 ) .

It follows that

(2.6) | w n ( r ) | 0 r | w n ( τ ) | d τ + | w n ( 0 ) | .

Thus, we have that

r N - 1 | w n ( r ) | K 0 r τ N - 1 | w n | 𝑑 τ
K 0 r τ N - 1 ( 0 τ | w n ( ς ) | d ς + | w n ( 0 ) | ) d τ
K 0 r τ N - 1 ( 0 r | w n ( ς ) | d ς + | w n ( 0 ) | ) d τ
K r N N 0 r | w n | d τ + K r N N | w n ( 0 ) | .

So we have that

| w n ( r ) | K N 0 r | w n | d τ + K N | w n ( 0 ) | .

The Gronwall–Bellman inequality shows that limn+wn(r)0. From (2.6), it follows that limn+wn(r)0. Therefore, we have that w(r)0 on [0,1], which contradicts w=1.

Next, we assume that r*>0. First, we consider r(0,r*]. It is easy to see that

w n ( r ) = - r r * w n ( τ ) 𝑑 τ + w n ( r * ) .

Therefore,

| w n ( r ) | r r * | w n ( τ ) | d τ + | w n ( r * ) | .

Then we have that

r N - 1 | w n ( r ) | K r r * τ N - 1 | w n | 𝑑 τ + ( r * ) N - 1 | w n ( r * ) |
K r r * τ N - 1 ( τ r * | w n ( ς ) | d ς + | w n ( r * ) | ) d τ + ( r * ) N - 1 | w n ( r * ) |
K r r * τ N - 1 ( r r * | w n ( τ ) | d τ + | w n ( r * ) | ) d τ + ( r * ) N - 1 | w n ( r * ) |
K r r * | w n ( τ ) | d τ r r * τ N - 1 d τ + K | w n ( r * ) | r r * τ N - 1 d τ + ( r * ) N - 1 | w n ( r * ) |
K r r * τ N - 1 r N - 1 | w n ( τ ) | 𝑑 τ r r * τ N - 1 𝑑 τ + K | w n ( r * ) | + | w n ( r * ) |
K r r * τ N - 1 | w n ( τ ) | 𝑑 τ 1 r N - 1 r r * τ N - 1 𝑑 τ + K | w n ( r * ) | + | w n ( r * ) |
K ( r * r ) N - 1 r r * τ N - 1 | w n | 𝑑 τ + K | w n ( r * ) | + | w n ( r * ) | .

By the Gronwall–Bellman inequality, we get that

r N - 1 | w n ( r ) | ( K | w n ( r * ) | + | w n ( r * ) | ) exp K ( r * r ) N - 1 ( r * - r ) .

This means that wn(r)0 on [0,r*] as n+. Similarly, for r[r*,1], we obtain that

r N - 1 | w n ( r ) | ( K | w n ( r * ) | + | w n ( r * ) | ) exp K ( r r * ) N - 1 ( r - r * ) .

It follows that wn(r)0 on [r*,1] as n+. It is obvious that

w n ( r ) = r * r w n ( τ ) 𝑑 τ + w n ( r * ) = w n ( ξ ) ( r - r * ) + w n ( r * ) 0 as n + ,

where ξ[r*,r] (or [r,r*]). Therefore, wn0 in C1 as n+, which is a contradiction. ∎

Now, by using the same argument as in the proof of [3, Lemma 1], we can show that λIk.

Proof of Theorem 1.

We only prove the case of 𝒞k+ because the case of 𝒞k- can be proved similarly. Let 𝒞k+ be the component of 𝒮k+(Ik×{0}) containing Ik×{0}. For any (λ,u)𝒞k+, there are two possibilities, either uSk+ or uSk+. Clearly, in the former case, (λ,u)Φk+. While, the latter case implies that u has at least one double zero in [0,1]. From Lemma 5, it follows that u0. Hence, there exists a sequence (λn,un)Φk+ such that (λn,un) is a solution of problem (1.2), and (λn,un) converges to (λ,0) in ×E. By Lemma 6, we have λIk, i.e., (λ,u)Ik×{0}. Hence, 𝒞k+(Φk+(Ik×{0})).

To complete the proof, it remains to show that 𝒞k+ is unbounded in ×E. Suppose, on the contrary, that 𝒞k+ is bounded. First, we claim that 𝒞k+ is compact in ×E. Consider, for a given hC[0,1], the following auxiliary problem:

(2.7) { - ( r N - 1 u ) = r N - 1 h ( r ) for a.e. r ( 0 , 1 ) , u ( 0 ) = u ( 1 ) = 0 .

It is well known that problem (2.7) can be equivalently written as u=G(h)(r), where G:C[0,1]E is continuous (see [8]). Define the Nemitskii operator H:×C[0,1]C[0,1] by

H ( λ , u ) ( r ) := λ u + f ( r , u , λ ) + g ( r , u , λ ) .

Then it is clear that H is a continuous operator and problem (1.2) can be equivalently written as

u = G H ( λ , u ) := Ψ ( λ , u ) .

Then Ψ:×EE is completely continuous. Hence, 𝒞k+ is compact in ×E because it is bounded. Applying a similar method as in the proof of [3, Theorem 1], with obvious changes, we may find an open bounded neighborhood 𝒪 of 𝒞k+ such that 𝒪𝒮k+=.

Now, we consider the approximate problem (2.1) again. For ϵ>0, it is easy to show that the nonlinear term f(r,u|u|ϵ,λ)+g(r,u,λ):=Fϵ(r,u,λ) satisfies the condition

lim s 0 F ϵ ( r , s , λ ) s = 0

uniformly in r[0,1] and on bounded λ intervals. Define the Nemitskii operator Hε:×C[0,1]C[0,1] by

H ε ( λ , u ) ( r ) := f ( r , u | u | ϵ , λ ) + g ( r , u , λ ) .

Then Hε is continuous and problem (2.1) can be equivalently written as

u = λ L ( u ) + H ~ ( λ , u ) ,

where L(u)=G(u), H~(λ,u)=GHε(λ,u). It is not difficult to verify that L:EE is linear completely continuous and H~:×EE is completely continuous with Φ=o(u) near u=0 uniformly on bounded λ sets. Let

𝒮 ϵ = { ( λ , u ) : ( λ , u ) satisfies (2.1) and u 0 } ¯ × E .

By [5, Theorem 2], there exist two continua 𝒞k,ϵ+ and 𝒞k,ϵ- of 𝒮ϵ, bifurcating from (λk,0), such that either 𝒞k,ϵ+ and 𝒞k,ϵ- are both unbounded or 𝒞k,ϵ+𝒞k,ϵ-{(λk,0)}. Theorem 4.1 of [8] shows that 𝒞k,ϵ+𝒞k,ϵ- is unbounded, lies in Φk and (𝒞k,ϵ+𝒞k,ϵ-)(×{0})={(λk,0)}. So 𝒞k,ϵ+ and 𝒞k,ϵ- are both unbounded and 𝒞k,ϵν(Φkν{(λk,0)}).

So there exists (λϵ,uϵ)𝒞k,ϵ+𝒪 for all ϵ>0. By compactness, one can find a sequence ϵn0 such that (λϵn,uϵn) converges to a solution (λ,u) of problem (1.2), and so uSk+¯. If uSk+, then by Lemma 5 we have u0. By Lemma 6, λIk, which contradicts the definition of 𝒪. On the other hand, if uSk+, then (λ,u)(𝒮k+𝒪) which contradicts 𝒪𝒮k+=. Therefore, 𝒞k+ is unbounded in ×E. ∎

3 Proofs of Theorem 2, and Corollaries 3 and 4

In this section, we consider the half-linear problem (1.3).

Proof of Theorem 2.

By Theorem 1, we know that there exists at least one solution of problem (1.3), (λkν,ukν)(×Skν), for every k=1,2,, and ν=±. The positive homogeneity of problem (1.3) implies that {(λkν,cukν),c>0} are half-linear solutions in {λkν}×Skν. Lemma 5 implies that any nontrivial solution u of problem (1.3) lies in some Skν.

We claim that for any solution (λ,u) of problem (1.3) with uSkν, we have that λ=λkν and u=cukν for some positive constant c. We may assume, without loss of generality, that the first zero of uukν to occur in (0,1] is a zero of u. That is, there exists ζ(0,1] such that u(ζ)=0, u and ukν do not vanish and have the same sign in (0,ζ). By [3, Lemma 3], one has that λkνλ. On the other hand, by [3, Lemma 2], there exists an interval (ξ,η)(0,1) such that u and ukν do not vanish and have the same sign in (ξ,η), and ukν(ξ)=ukν(η)=0. Again, by [3, Lemma 3], λλkν. Hence, λ=λkν.

Next, we shall prove that u=cukν for some positive constant c. Without loss of generality, we may assume that u and ukν are positive in (0,ζ). By some simple calculations, noting λ=λkν, we have that

(3.1) - 0 ζ ( u 2 r N - 1 ( u k ν ) u k ν - u ( r N - 1 u ) ) 𝑑 r = Γ 3 ,

where

Γ 3 = 0 ζ r N - 1 ( | u | 2 + | u ( u k ν ) u k ν | 2 - 2 u u ( u k ν ) u k ν ) 𝑑 r .

The left-hand side of (3.1) equals

lim r 0 + u 2 r N - 1 ( u k ν ) u k ν - lim r ζ - u 2 r N - 1 ( u k ν ) u k ν := H 0 - H ζ .

Lemma 5 implies that ukν(0)0, and thus H0=0. If ukν(ζ)0, then Hζ=0. Otherwise, one has (ukν)(ζ)0. By the L’Hospital rule, we have that

H ζ = lim r ζ - u 2 r N - 1 ( u k ν ) u k ν
= lim r ζ - 2 u u r N - 1 ( u k ν ) + u 2 ( r N - 1 ( u k ν ) ) ( u k ν )
= lim r ζ - 2 u u r N - 1 ( u k ν ) - u 2 r N - 2 ( λ k ν u k ν + α u k ν ) ( u k ν )
= 0 .

Therefore, the left-hand side of (3.1) equals zero. Hence, the right-hand side of (3.1) also equals zero. It follows that u=c1ukν on [0,ζ] for some positive constant c1. We may assume, without loss of generality, that the first zero of uukν to occur in (ζ,1] is a zero of u. That is, there exists ζ1(ζ,1] such that u(ζ1)=0, and u and ukν do not vanish and have the same sign in (ζ,ζ1). Reasoning as above, we can show that u=c2ukν on [ζ,ζ1] for some positive constant c2. Clearly, u(ζ)=c1(ukν)(ζ)=c2(ukν)(ζ), and Lemma 5 implies c1=c2. Repeating the above process k times, we can show that u=cukν for some positive constant c.

Finally, we show that the sequences λkν (ν=±) are increasing. Given solutions (λkν,u) and (λjν,v) with uSkν, vSjν and k<j, the first zero of uv to occur in (0,1) is a zero of v. Indeed, if this was not the case, using the same argument as above, Lemmas 2 and 3 of [3] imply λkν=λjν, which is impossible, since the half-eigenvalues were shown to be simple. Therefore, by [3, Lemma 3], we have that λkν<λjν. ∎

Proof of Corollary 4.

We suppose, on the contrary, that λj-=λi+ for some i, j with ij. Firstly, we shall prove that -φj-=φi+ for some positive constant c. Without loss of generality, we may assume that the first zero of -φj-φi+ to occur in (0,1] is a zero of φj-. That is, there exists ξ(0,1] such that φj-(ξ)=0, -φj- and φi+ are positive in (0,ξ). By some simple calculations, noting λj-=λi+, we have that

(3.2) - 0 ξ ( ( φ j - ) 2 r N - 1 ( φ i + ) φ i + - φ j - ( r N - 1 ( φ j - ) ) ) 𝑑 r = Γ 4 ,

where

Γ 4 = 0 ξ r N - 1 ( | ( φ j - ) | 2 + | φ j - ( φ i + ) φ i + | 2 - 2 φ j - ( φ j - ) ( φ i + ) φ i + ) 𝑑 r .

The left-hand side of (3.2) equals

lim r 0 + ( φ j - ) 2 r N - 1 ( φ i + ) φ i + - lim r ξ - ( φ j - ) 2 r N - 1 ( φ i + ) φ i + := H 0 - H ξ .

Lemma 5 implies that φi+(0)0, and thus H0=0. If φi+(ξ)0, then Hξ=0. Otherwise, one has (φi+)(ξ)0. By the L’Hospital rule, we have that

H ξ = lim r ξ - ( φ j - ) 2 r N - 1 ( φ i + ) φ i +
= lim r ξ - 2 φ j - ( φ j - ) r N - 1 ( φ i + ) + ( φ j - ) 2 ( r N - 1 ( φ i + ) ) ( φ i + )
= lim r ξ - 2 φ j - ( φ j - ) r N - 1 ( φ i + ) - ( φ j - ) 2 r N - 1 ( λ i + φ i + + α φ i + ) ( φ i + )
= 0 .

Therefore, the left-hand side of (3.2) equals zero. Hence, the right-hand side of (3.2) also equals zero. It follows that -φj-=c1φi+ on [0,ξ] for some positive constant c1. We may assume, without loss of generality, that the first zero of -φj-φi+ to occur in (ξ,1] is a zero of φj-. That is, there exists ξ1(ξ,1] such that φj-(ξ1)=0, and -φj- and φi+ do not vanish and have the same sign in (ξ,ξ1). Reasoning as above, we can show that -φj-=c2φi+ on [ξ,ξ1] for some positive constant c2. Clearly, (-φj-)(ξ)=c1(φi+)(ξ)=c2(φi+)(ξ) and Lemma 5 imply c1=c2. Repeating the above process at most j+i times, we can show that -φj-=cφi+ for some positive constant c. In fact, the constant c is 1 because φiν=1, but this is not possible because Si+Sj+=. ∎

Proof of Corollary 3.

From the argument of Corollary 4, we know that φi-=-φi+ for some positive constant c if λi-=λi+. So -φi+ is an eigenfunction corresponding to λi+. It follows that

( α ( r ) + β ( r ) ) | φ i + ( r ) | 0 , r ( 0 , 1 ) .

So we get β(r)-α(r) in (0,1)Zi, which is a contradiction. ∎

Remark 7

If β(r)-α(r) in (0,1)Zk, then (λk+,-φk+) is an eigenpair of problem (1.3). Then, using a similar argument as in the proof of Theorem 2, we can show that λk+=λk- and -φk+=φk- because -φk+Sk-.


Communicated by Paul Rabinowitz


Award Identifier / Grant number: 11261052

Award Identifier / Grant number: 11401477

Funding statement: The first author acknowledges the support of NNSF of China (nos. 11261052 and 11401477), the Fundamental Research Funds for Central Universities (no. DUT15RC(3)018), Scientific Research Project of the Higher Education Institutions of Gansu Province (no. 2014A-009) and Research Project of Science and Technology of Liaoning Provincial Education Department (no. ZX20150135).

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Received: 2014-12-18
Revised: 2015-05-11
Accepted: 2016-06-16
Published Online: 2016-09-02
Published in Print: 2016-11-01

© 2016 by De Gruyter

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