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Global structure of sign-changing solutions for discrete Dirichlet problems

  • Liping Wei and Ruyun Ma EMAIL logo
Published/Copyright: June 18, 2020

Abstract

Let T > 1 be an integer, T [ 1 , T ] Z = { 1 , 2 , , T } , T ˆ { 0 , 1 , , T + 1 } . In this article, we are concerned with the global structure of the set of sign-changing solutions of the discrete second-order boundary value problem

{ Δ 2 u ( x 1 ) + λ h ( x ) f ( u ( x ) ) = 0 , x T , u ( 0 ) = u ( T + 1 ) = 0 ,

where λ > 0 is a parameter, f C ( , ) satisfies f ( 0 ) = 0 , s f ( s ) > 0 for all s 0 and h : T ˆ [ 0 , + ) . By using the directions of a bifurcation, we obtain existence and multiplicity of sign-changing solutions of the above problem for λ lying in various intervals in . Moreover, we point out that these solutions change their sign exactly k 1 times, where k { 1 , 2 , , T } .

MSC 2010: 39A70; 39A28; 47A75

1 Introduction

In this article, we are concerned with the discrete second-order boundary value problem

(1.1) { Δ 2 u ( x 1 ) + λ h ( x ) f ( u ( x ) ) = 0 , x T , u ( 0 ) = u ( T + 1 ) = 0 ,

where T [ 1 , T ] Z = { 1 , 2 , , T } , T > 1 is an integer, T ˆ { 0 , 1 , , T + 1 } , λ > 0 is a parameter and h , f satisfy the following assumptions.

(A1) h : T ˆ [ 0 , + ) with 0 < h h ( t ) h on T ˆ for some h , h ( 0 , ) .

In assumption (A2) and throughout the article, we use the following well-known conceptions of a generalized zero and a simple generalized zero at t T .

Definition 1.1

Suppose that a function y : T ˆ . If y ( t 0 ) = 0 , then t 0 is a zero of y. If y ( t 0 ) = 0 or y ( t 0 ) y ( t 0 + 1 ) < 0 for some t 0 { 1 , , T 1 } , then y has a generalized zero at t 0 T .

Definition 1.2

A function y : T ˆ is said to have a simple generalized zero at t 0 T provided that one of the following conditions is satisfied:

  1. y ( t 0 ) = 0 , y ( t 0 1 ) y ( t 0 + 1 ) < 0 ;

  2. y ( t 0 ) y ( t 0 + 1 ) < 0 .

It is well-known that the eigenvalue problem

(1.2) { Δ 2 u ( x 1 ) + μ h ( x ) u ( x ) = 0 , x T , u ( 0 ) = u ( T + 1 ) = 0

has a finite sequence of simple eigenvalues

0 < μ 1 < μ 2 < < μ T ,

and the eigenfunction ϕ k corresponding to μ k has exactly k 1 simple generalized zeros in T (see [1], and for other spectral results of related problems we refer to [2]). Let

0 = t 0 < t 1 < < t k 1 < t k = T + 1

be the generalized zeros of ϕ k .

In the special case h ( x ) 1 , the mth eigenvalue and eigenfunction corresponding to it are characterized by

η m = 2 2 cos m π T + 1 , ψ m ( t ) = sin ( m T + 1 π t ) ,

respectively. Let

0 = τ 0 < τ 1 < < τ m 1 < τ m = T + 1

be the generalized zeros of sin ( m T + 1 π t ) in T ˆ . Then,

τ j + 1 τ j { t Z | T + 2 m m t T + m m } , j { 0 , 1 , , m 1 } .

We assume that

(A2) there exist two constants m 1 , m 2 { 1 , 2 , , T } , such that

(1.3) η m 1 μ k h ( t ) max s ( 0 , ) f ( s ) s η m 2 , t T ˆ

for some k .

From (1.3) and the Sturm-type comparison theorem, see Aharonov, Bohner and Elias [3], there exists c = min { t Z | T + 2 m 2 m 2 t T + m 2 m 2 } , such that

t j + 1 t j c , j { 0 , 1 , , k 1 } .

Let χ 1 be the principal eigenvalue of the eigenvalue problem

(1.4) { Δ 2 w ( x 1 ) + χ w ( x ) = 0 , x [ 1 , c ˆ 1 ] Z , w ( 0 ) = w ( c ˆ ) = 0 ,

where c ˆ T satisfies c 2 c ˆ c + 1 2 , and let w 1 be an eigenfunction corresponding to χ 1 .

Furthermore, we assume that

(A3) there exist α > 0 , f 0 > 0 and f 1 > 0 such that

lim | s | 0 f ( s ) f 0 s s | s | α = f 1 ;

(A4) f C ( , ) , f ( 0 ) = 0 , s f ( s ) > 0 for s 0 and f lim | s | f ( s ) s = 0 ;

(A5) there exist s 0 > 0 and 0 < σ < 1 such that

min | s | [ s 0 , 1 σ s 0 ] f ( s ) s f 0 μ k h χ 1 .

In order to state our main result, we first recall some standard notations to describe the properties of sign-changing solutions. Let Y = { u | u : T } with the norm u Y = max t T | u ( t ) | . Let X = { u : T ˆ | u ( 0 ) = u ( T + 1 ) = 0 } with the norm u = max t T ˆ | u ( t ) | . For k 1 , ν { + , } , let S k ν denote the set of functions in X such that

  1. u has exactly k 1 simple generalized zeros in T ;

  2. ν u ( 1 ) > 0 .

Define S k = S k S k + . They are disjoint and open in X. Finally, let Φ k ± = × S k ± and Φ k = × S k . A S k ν solution of (1.1) is a function u S k ν satisfying (1.1).

Our main result is the following.

Theorem 1.3

For each fixed integer k { 1 , 2 , , T } and each fixed ν { + , } , let (A1)–(A5) hold. Then, there exist λ ( 0 , μ k / f 0 ) and λ > μ k / f 0 , such that

  1. (1.1) has at least one S k ν solution if λ = λ ;

  2. (1.1) has at least two S k ν solutions if λ < λ μ k / f 0 ;

  3. (1.1) has at least three S k ν solutions if μ k / f 0 < λ < λ ;

  4. (1.1) has at least two S k ν solutions if λ = λ ;

  5. (1.1) has at least one S k ν solution if λ > λ .

Existence and multiplicity of positive solutions for discrete boundary value problems have been extensively studied by several authors. We refer to Agarwal et al. [4,5], Cheng and Yen [6], Rachunkova and Tisdell [7], Ma [8], Rodriguez [9] and references therein. However, the methods in [4,5,6,7,8,9] are analytic techniques and various fixed point theorems, which cannot be used to prove the existence of S k ν solutions.

By using the global bifurcation theory [10,11], Davidson and Rynne [12] and Luo and Ma [13] studied second-order Dirichlet boundary value problems on measure chain. It is well-known that measure chain T ˜ denotes an arbitrary closed subset of real numbers , and we can regard the equations in [12,13] as difference equations when T ˜ = Z . They showed that unbounded continua of nontrivial solutions prescribed nodal properties emanated from the trivial branch at the eigenvalues of the linearization problems. However, they only showed that for each fixed integer k 1 and ν { + , } , there exists at least one nodal solution.

Remark 1.4

Existence of c ˆ in (1.4) can be guaranteed by (A2). For example, let T = 100 , m 2 = 5 . By using Mathematica 9.0, the distance between two consecutive generalized zeros of ψ m 2 ( t ) was found to be 20, which means c = 20 . Thus, it is easy to check that c ˆ = 10 by the definition of c ˆ .

The rest of the article is organized as follows. In Section 2, we show the existence of bifurcation from some eigenvalues for the corresponding problem according to the standard argument and the rightward direction of bifurcation. In Section 3, the change in direction of bifurcation is given. The final section is devoted to show an a priori bound of solutions for (1.1) and complete the proof of Theorem 1.3.

2 Rightward bifurcation

We study the global behavior from the trivial branch with the rightward direction of bifurcation under suitable assumptions on h and f.

Lemma 2.1

Suppose that ( λ , u ) is a nontrivial solution of ( 1.1 ). Then, there exists k 0 { 1 , 2 , , T } , such that

u S k 0 ν .

Proof

Suppose on the contrary that for every k { 1 , 2 , , T } ,

u S k ν .

Then, there exists t 0 T such that

(2.1) u ( t 0 ) = 0 , u ( t 0 1 ) u ( t 0 + 1 ) 0 .

Since u ≢ 0 on T ˆ , we may assume that

(2.2) | u ( t 0 1 ) | + | u ( t 0 + 1 ) | > 0 .

On the other hand, it follows from equation (1.1) and f ( 0 ) = 0 that

Δ 2 u ( t 0 1 ) = λ h ( t 0 ) f ( u ( t 0 ) ) = 0 ,

which implies that

u ( t 0 + 1 ) 2 u ( t 0 ) + u ( t 0 1 ) = 0 .

However, by (2.2) and the fact u ( t 0 ) = 0 , we get

(2.3) u ( t 0 + 1 ) u ( t 0 1 ) < 0 ,

which contradicts (2.1).□

Next following the similar arguments in Gao and Ma [14], with obvious changes, we may get the following.

Lemma 2.2

Assume that (A1), (A3) and (A4) hold. Let (A2) be satisfied for some k . Then for each ν { + , } , there exists an unbounded subcontinuum C k ν which is branching from ( μ k / f 0 , 0 ) for ( 1.1 ). Moreover, if ( λ , u ) C k ν , then u is a S k ν solution of ( 1.1 ).

Lemma 2.3

Assume that (A1), (A3) and (A4) hold. Let (A2) be satisfied for some k . Let u be a S k ν solution of ( 1.1 ). Then, there exists a constant C > 0 independent of u such that

(2.4) | Δ u ( x ) | λ C u , x [ 0 , T ] Z .

Proof

According to discrete Rolle’s theorem (see [1]), there exists x 0 T , such that Δ u ( x 0 ) = 0 or Δ u ( x 0 1 ) Δ u ( x 0 ) < 0 . Then by a direct computation, it is easy to see that

(2.5) Δ u ( x ) = Δ u ( x 0 ) + λ s = x + 1 x 0 h ( s ) f ( u ( s ) ) , x T .

Noting that (A3) and (A4) imply that

(2.6) | f ( s ) | f | s | , s

for some f > 0 , it follows from (2.5) that

  1. if Δ u ( x 0 ) = 0 , then

    | Δ u ( x ) | = λ s = x + 1 x 0 | h ( s ) f ( u ( s ) ) | λ f u s = x + 1 x 0 h ( s ) λ f s = 0 T + 1 h ( s ) u ;

  2. if Δ u ( x 0 1 ) Δ u ( x 0 ) < 0 , then

| Δ u ( x ) | = | Δ u ( x 0 ) + λ s = x + 1 x 0 h ( s ) f ( u ( s ) ) | ( 2 + λ f s = 0 T + 1 h ( s ) ) u .

Lemma 2.4

Assume that (A1), (A3) and (A4) hold. Let (A2) be satisfied for some k . Let { ( λ n , u n ) } be a sequence of S k ν solutions to ( 1.1 ), which satisfies u n 0 and λ n μ k / f 0 . Let ϕ k ( x ) be the kth eigenfunction of ( 1.2 ), which satisfies ϕ k = 1 . Then, there exists a subsequence of { u n } , again denoted by { u n } , such that u n / u n converges uniformly to ϕ k on T .

Proof

Set v n u n / u n . Then, it is easy to see that v n = 1 . It follows from Lemma 2.3 that Δ v n is bounded, so there is a subsequence of v n uniformly convergent to a limit v. Furthermore, there exists a subsequence of it such that Δ v n ( 0 ) converges to some constant c. We again denote by v n the subsequence. We note that v Y , v ( 0 ) = v ( T + 1 ) = 0 and v = 1 . Rewriting equation (1.1) with ( λ , u ) = ( λ n , u n ) , we obtain

(2.7) Δ u n ( x ) = Δ u n ( 0 ) λ n t = 1 x h ( t ) f ( u n ( t ) ) .

Dividing both sides of (2.7) by u n , we get

(2.8) Δ v n ( x ) = Δ v n ( 0 ) λ n t = 1 x h ( t ) f ( u n ( t ) ) u n ( t ) v n ( t ) w n ( x ) .

Noting that u n ( x ) 0 for all x T ˆ , so for each fixed t T ˆ , one has f ( u n ( t ) ) u n ( t ) f 0 . It follows from (2.6) that w n ( x ) converges to

(2.9) w ( x ) c μ k t = 1 x h ( t ) v ( t )

for each fixed x T ˆ . Therefore, by recalling (2.8), one has

v n ( x ) = s = 1 x 1 w n ( s ) .

The fact coupled with (2.9) yields that v n ( x ) converges to

v ( x ) = s = 1 x 1 ( c μ k t = 1 s h ( t ) v ( t ) ) ,

which implies that v is a nontrivial solution of (1.2) with λ = μ k , and hence v ϕ k .□

Lemma 2.5

Assume that (A1), (A3) and (A4) hold. Let (A2) be satisfied for some k . Let C k ν be as in Lemma 2.2. Then there exists δ > 0 such that for ( λ , u ) C k ν and | λ μ k / f 0 | + u δ , one has λ > μ k / f 0 .

Proof

Suppose on the contrary that there exists a sequence { ( λ n , u n ) } such that ( λ n , u n ) C k ν , which satisfies λ n μ k / f 0 , u n 0 and λ n μ k / f 0 . According to Lemma 2.4, there exists a subsequence of { u n } , for convenience denote it by { u n } , such that u n u n converges uniformly to ϕ k on T ˆ , where ϕ k ( x ) S k ν is the kth eigenfunction of (1.2) with ϕ k = 1 . Multiplying the equation of (1.1) with ( λ , u ) = ( λ n , u n ) by u n and by a direct computation, one has

λ n x = 0 T h ( x ) f ( u n ( x ) ) u n ( x ) = x = 0 T | Δ u n ( x ) | 2 ,

and accordingly

(2.10) λ n x = 0 T h ( x ) f ( u n ( x ) ) u n u n ( x ) u n = x = 0 T | Δ u n ( x ) | 2 u n 2 .

It follows from Lemma 2.4 that after taking a subsequence and relabeling if necessary, u n u n converges to ϕ k in Y.

x = 0 T | Δ ϕ k ( x ) | 2 = μ k x = 0 T h ( x ) | ϕ k ( x ) | 2 ,

then coupled with (2.10), one has

λ n x = 0 T h ( x ) f ( u n ( x ) ) u n ( x ) = μ k x = 0 T h ( x ) | u n ( x ) | 2 ζ ( n ) u n 2

with a function ζ : satisfying

lim n ζ ( n ) = 0 .

That is,

x = 0 T + 1 h ( x ) f ( u n ( x ) ) f 0 u n ( x ) | u n ( x ) | α u n ( x ) | u n ( x ) u n | 2 + α = 1 λ n u n α [ ( μ k f 0 λ n ) x = 0 T + 1 h ( x ) | u n ( x ) u n | 2 ζ ( n ) ] .

From condition (A3), we have

x = 0 T + 1 h ( x ) f ( u n ( x ) ) f 0 u n ( x ) | u n ( x ) | α u n ( x ) | u n ( x ) u n | 2 + α f 1 x = 0 T + 1 h ( x ) | ϕ k ( x ) | 2 + α < 0 ,

and

x = 0 T + 1 h ( x ) | u ( x ) u n | 2 x = 0 T + 1 h ( x ) | ϕ k ( x ) | 2 > 0 .

This contradicts λ n μ k / f 0 .□

3 Direction turn of bifurcation

In this section, we show that the connected components grow to the left at some point under (A5) condition.

Lemma 3.1

Assume that (A2) holds for some k . Let u be a S k ν solution of (1.1). Then there exist two generalized zeros α u and β u , such that

β u α u c ,

| u | > 0 , x [ α u + 1 , β u 1 ] Z ,

u = | u ( t 0 ) | for some t 0 [ α u , β u ] Z .

Moreover,

σ u | u ( x ) | u , x { t Z : 3 α u + β u 4 t α u + 3 β u 4 } J u ,

where σ = min { min J u β u α u , β u max J u β u α u } .

Proof

It is an immediate consequence of the fact that u is concave down in T ˆ .□

Lemma 3.2

Assume that (A1) and (A5) hold. Let σ be as in Lemma 3.1 and u be a S k ν solution of (1.1) with u = 1 σ s 0 . Then λ < μ k / f 0 .

Proof

Let u be a S k ν solution of (1.1). It follows from Lemma 3.1 that

σ u | u ( x ) | u , x J u .

We note that u is a solution of

Δ 2 u ( x ) + λ h ( x ) f ( u ( x ) ) u ( x ) u ( x ) = 0 , x J u .

Suppose on the contrary that λ μ k / f 0 . Then for x J u , we have from (A5) that

λ h ( x ) f ( u ( x ) ) u ( x ) μ k f 0 h f 0 μ k h χ 1 = χ 1 .

Choose b > 0 , such that [ b , b + c ˆ ] Z J u . Set

y ( x ) = w 1 ( x b ) , x [ b , b + c ˆ ] Z ,

then

{ Δ 2 y ( x 1 ) + χ 1 y ( x ) = 0 , x [ a , b ] Z , y ( b ) = y ( b + c ˆ ) = 0 .

Combine this with a generalized version of the Sturm-type comparison theorem [3]. We deduce that u has at least one generalized zero on J u . This contradicts the fact that u ( x ) > 0 on J u .□

4 Second turn and proof of Theorem 1.3

The main ingredient of this section is an a priori estimate and finally we shall give a proof of Theorem 1.3.

Lemma 4.1

Assume that (A3) and (A4) hold. Let ( λ , u ) be a S k ν solution of (1.1). Then, there exists λ > 0 such that λ λ .

Proof

From Lemma 2.3, there exists a constant C > 0 , which is independent of u such that (2.4) holds. Let u = u ( x 0 ) , then it follows from (2.4) that

(4.1) u = | u ( x 0 ) | = s = 0 x 0 1 Δ u ( s ) s = 0 x 0 1 λ C u λ C T u ,

that is, λ ( C T ) 1 .□

Lemma 4.2

Assume that (A1) and (A4) hold. Let (A2) be satisfied for some k . Let u be an S k ν solution of ( 1.1 ). Then, there exists a constant C > 0 independent of u such that for f ̲ ( s ) = min σ s t s f ( t ) / t , one has λ f ̲ ( u ) C .

Proof

Let

0 = t 0 < t 1 < < t k = T + 1

be the generalized zeros of u. Then, by (A2) we may get

t j + 1 t j c , j { 0 , 1 , , k 1 } .

We may assume that

(4.2) u = u ( x 0 ) , x 0 t l , t l + 1 Z ,

or

(4.3) u = u ( x 0 ) , x 0 t l , t l + 1 Z .

We only deal with case (4.2) since case (4.3) can be treated by the similar way.

Let

J l = { t Z : 3 t l + t l + 1 4 t t l + 3 t l + 1 4 } .

Let t ˆ T satisfy t l + 1 t l 2 t ˆ t l + 1 t l + 1 2 and

J 1 [ min J l , t ˆ ] , J 2 [ t ˆ , max J l ] .

If u ( t l ) = u ( t l + 1 ) = 0 , then it follows from (4.2) that

u | u ( t ˆ ) | = λ s = t l t l + 1 [ G ( t ˆ , s ) h ( s ) f ( u ( s ) ) ] = λ u s = t l t l + 1 [ G ( t ˆ , s ) h ( s ) f ( u ( s ) ) u ] λ u s J l [ G ( t ˆ , s ) h ( s ) min σ u r u f ( r ) r u ( s ) u ] σ λ u s J l [ G ( t ˆ , s ) h ( s ) f ̲ ( u ) ] σ λ u f ̲ ( u ) h ( t l + 1 t l ) min s J l { G ( t ˆ , s ) : s J l } ,

where

G ( t ˆ , s ) = 1 T + 1 { ( T + 1 t ˆ ) s , 0 s t ˆ T + 1 , ( T + 1 s ) t ˆ , 0 t ˆ s T + 1 .

If u ( t l ) = A 0 , u ( t l + 1 ) = B 0 , then it follows from (4.2) again that

u | u ( t ˆ ) | = | u ˜ ( t ˆ ) + λ s = t l t l + 1 [ G ( t ˆ , s ) h ( s ) f ( u ( s ) ) ] | λ | s = t l t l + 1 [ G ( t ˆ , s ) h ( s ) f ( u ( s ) ) ] | | u ˜ ( t ˆ ) | λ | s = t l t l + 1 [ G ( t ˆ , s ) h ( s ) f ( u ( s ) ) ] | u ,

where u ˜ ( t ˆ ) is the solution of Δ 2 u ˜ ( t ˆ 1 ) = 0 with boundary value condition u ˜ ( t l ) = A , u ˜ ( t l + 1 ) = B . Then by the similar argument as above, we complete the proof.□

Lemma 4.3

Assume that (A1) and (A3) hold, (A2) be satisfied for some k . Let J be a compact interval in ( 0 , ) . Then, there exists a constant M J > 0 such that for all λ J and given ν { + , } , one has all possible S k ν solutions u of (1.1) satisfy u M J .

Proof

Suppose on the contrary that there exists a sequence { u n } of S k ν solutions of (1.1) with { λ n } J [ a , b ] and u n as n . Then by the same argument used in the proof of Lemma 4.2, with obvious changes, we may get

u n = u n ( x 0 ) , x 0 t m , t m + 1 Z .

Let

ρ ( 0 , 1 b Q ) ,

where Q = s = 1 T G ( t , s ) h ( s ) . Then by (A3), there exists u ρ > 0 such that u > u ρ implies f ( u ) < ρ u .

Let m ρ max u [ 0 , u ρ ] f ( u ) and let A n { t [ t m , t m + 1 ] Z : u n ( t ) u ρ } and B n { t [ t m , t m + 1 ] Z : u n ( t ) > u ρ } . Then we have,

u n ( δ n ) = u ˜ ( δ n ) + s = t m + 1 t m + 1 λ n G ( δ n , s ) h ( s ) f ( u n ( s ) ) = u ˜ ( δ n ) + s A n λ n G ( δ n , s ) h ( s ) f ( u n ( s ) ) + s B n λ n G ( δ n , s ) h ( s ) f ( u n ( s ) )

for 0 s δ n . Thus,

1 λ n u ˜ ( δ n ) λ n u n + m ρ Q u n + s B n G ( δ n , s ) h ( t ) f ( u n ( t ) ) u n .

On B n , u n ( s ) > u ρ implies f ( u n ( s ) ) u n f ( u n ( s ) ) u n ( s ) ρ . Accordingly,

1 λ n u ˜ ( δ n ) λ n u n + m ρ Q u n + ρ Q .

Since 0 < a < λ n b for all n, we have 1 b 1 λ n 1 a for all n and

1 b < u ˜ ( δ n ) a u n + m ρ Q u n + ρ Q .

According to the fact u n as n , we get

1 b < ρ Q < 1 b .

This contradiction completes the proof.□

Lemma 4.4

Assume that (A1), (A3) and (A4) hold. Let (A2) hold for some k . Then there exists { ( λ n , u n ) } such that ( λ n , u n ) C k ν , λ n as n and u n .

Proof

We only deal with the case ν = + .

It follows from Lemma 2.2 that C k ν is unbounded, so there exists a sequence { ( λ n , u n ) } of solutions of (1.1) such that { ( λ n , u n ) } + × S k + and | λ n | + u n . Moreover, Lemma 4.1 implies that λ n > 0 . Suppose on the contrary that there exists a bounded subsequence { ( λ n k , u n k ) } . Then from Lemma 4.3, u n k is bounded, which contradicts the fact that | λ n | + u n . So, λ n . Then, Lemma 4.2 implies that f ̲ ( u n ) 0 . It deduces from (A4) that u n .□

Proof of Theorem 1.3

Let C k ν be as in Lemma 2.2. In order to simplify the proof, we only deal with the case C k + .

It follows from Lemma 2.5 that C k + is branching from ( μ k / f 0 , 0 ) and goes rightward. Let { ( λ n , u n ) } be as in Lemma 4.4. Then, there exists ( λ 0 , u 0 ) C k + such that u 0 = 1 σ s 0 . By Lemma 3.2, one has λ 0 < μ k / f 0 .

Coupled with Lemmas 2.5, 3.2 and 4.3, C k + passes through some points ( μ k / f 0 , v 1 ) and ( μ k / f 0 , v 2 ) with

v 1 < 1 σ s 0 < v 2 .

By Lemmas 2.5, 3.2 and 4.3 again, there exist λ ̲ and λ ¯ , which satisfy 0 < λ ̲ < μ k / f 0 < λ ¯ and

  1. if λ ( μ k / f 0 , λ ¯ ] , then there exist u and v such that ( λ , u ) , ( λ , v ) C k + and

    u < v < 1 σ s 0 ;

  2. if λ [ λ ̲ , μ k / f 0 ] , then there exist u and v such that ( λ , u ) , ( λ , v ) C k + and

u < 1 σ s 0 < v .

Define

λ = sup { λ ¯ : λ ¯ satisfies ( i ) } , λ = inf { λ ̲ : λ ̲ satisfies ( ii ) } .

Then by the standard argument, (1.1) has a S k + solution at λ = λ and λ = λ , respectively. Lemma 3.2 implies that there exists w such that for each λ > μ k / f 0 , one has ( λ , w ) C k ν and w > 1 σ s 0 . This completes the proof.□

Acknowledgements

The authors are very grateful to the anonymous referees for their valuable suggestions.

  1. Funding: This work was supported by the National Natural Science Foundation of China (No. 11671322).

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Received: 2019-10-18
Revised: 2020-03-03
Accepted: 2020-04-28
Published Online: 2020-06-18

© 2020 Liping Wei and Ruyun Ma, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  3. Strong and weak convergence of Ishikawa iterations for best proximity pairs
  4. Curve and surface construction based on the generalized toric-Bernstein basis functions
  5. The non-negative spectrum of a digraph
  6. Bounds on F-index of tricyclic graphs with fixed pendant vertices
  7. Crank-Nicolson orthogonal spline collocation method combined with WSGI difference scheme for the two-dimensional time-fractional diffusion-wave equation
  8. Hardy’s inequalities and integral operators on Herz-Morrey spaces
  9. The 2-pebbling property of squares of paths and Graham’s conjecture
  10. Existence conditions for periodic solutions of second-order neutral delay differential equations with piecewise constant arguments
  11. Orthogonal polynomials for exponential weights x2α(1 – x2)2ρe–2Q(x) on [0, 1)
  12. Rough sets based on fuzzy ideals in distributive lattices
  13. On more general forms of proportional fractional operators
  14. The hyperbolic polygons of type (ϵ, n) and Möbius transformations
  15. Tripled best proximity point in complete metric spaces
  16. Metric completions, the Heine-Borel property, and approachability
  17. Functional identities on upper triangular matrix rings
  18. Uniqueness on entire functions and their nth order exact differences with two shared values
  19. The adaptive finite element method for the Steklov eigenvalue problem in inverse scattering
  20. Existence of a common solution to systems of integral equations via fixed point results
  21. Fixed point results for multivalued mappings of Ćirić type via F-contractions on quasi metric spaces
  22. Some inequalities on the spectral radius of nonnegative tensors
  23. Some results in cone metric spaces with applications in homotopy theory
  24. On the Malcev products of some classes of epigroups, I
  25. Self-injectivity of semigroup algebras
  26. Cauchy matrix and Liouville formula of quaternion impulsive dynamic equations on time scales
  27. On the symmetrized s-divergence
  28. On multivalued Suzuki-type θ-contractions and related applications
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  30. Two types of hypergeometric degenerate Cauchy numbers
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  56. Asymptotic relations for the products of elements of some positive sequences
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