Citation: Xianyong Yang, Zhipeng Yang. Existence of multiple non-trivial solutions for a nonlocal problem[J]. AIMS Mathematics, 2019, 4(2): 299-307. doi: 10.3934/math.2018.2.299
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In this paper, we study the following general nonlocal equation
{−LKu=λ1u+f(x,u)in Ω,u=0in RN∖Ω, | (1.1) |
where Ω⊂RN is open, bounded domain with smooth boundary, λ1 is the first eigenvalue of the nonlocal integro-differential operator LK, which is defined by (see [1])
LKu(x):=∫RN[u(x+y)+u(x−y)−2u(x)]K(y)dy,x∈RN, | (1.2) |
where K:RN∖{0}→(0,+∞) satisfies the following conditions:
(K1) γK∈L1(RN),whereγ(x)=min{|x|2,1}
(K2) there exists δ>0 such that K(x)≥δ|x|−(N+2s),∀x∈RN.
We remark that the Dirichlet datum is given in RN∖Ω and not simply on ∂Ω, consistently with the non-local character of the operator LK.
A typical example for the function K(x) is K(x)=|x|−(N+2s), then the operator LK reduce to the so-called fractional Laplacian operator (−Δ)s and (1.1) reduce to
{(−Δ)su=λ1u+f(x,u)in Ω,u=0in RN∖Ω, | (1.3) |
which plays an increasingly significant role in both pure mathematical research and concrete applications, such as the thin obstacle problem [2,3], minimal surfaces [4,5], phase transitions [6], anomalous diffusion [7,8,9] and mathematical finance [10]. See [11,12,13,14,15] and references therein for an elementary introduction to the literature.
Different than the classical Laplacian operator −Δ, the fractional Laplacian operator (−Δ)s is known to be nonlocal and this difference may cause some difficulties to implement by variational methods. Over the past decades, problems similar to (1.1) have roused enough interest, many scholars have shown their concern in elliptic equation for bounded domains and unbounded domains, see [16,17,18,19,20,21,22] and the references therein.
On the other hand, there are few results concerned with the general nonlocal problem with the operator LK. In [1,23], the authors study problem (1.1) by both the mountain pass theorem and the linking theorem. In [24], the authors obtained a Brezis-Nirenberg result for the operator LK. Infinitely many positive solutions and sign-changing solutions have been studied in [25,26]. For other results about the operator LK we refer to [12,27] and their references therein.
Problem (1.1) has a variational character and the natural space where finding weak solutions for it is the functional space X, defined as follows (for more details we refer to [1] and [23], where this space was introduced and some properties of this space were proved).
Let
X:={u:RN→R|uis Lebesgue measurable,u|Ω∈L2(Ω)and∫Q(u(x)−u(y))2K(x−y)dxdy<∞}, |
where Q=R2N∖(CΩ×CΩ), CΩ:=RN∖Ω. The space X is endowed with the following norm
‖u‖X=|u|2+[u]X, |
and
[u]X=(∫Q|u(x)−u(y)|2K(x−y)dxdy)12. |
We can easily check that ‖⋅‖X is a norm on X. Define
E:={u∈X:u=0a.e.inRN∖Ω}. |
From [1,23], we have the following Poincaré type inequality: there exists a constant C>0 such that for all u∈E,
|u|2≤C[u]X. |
Moreover, the norm
‖u‖:=[u]X=(∫Q|u(x)−u(y)|2K(x−y)dxdy)1/2=(∫R2N|u(x)−u(y)|2K(x−y)dxdy)1/2 |
is an equivalent norm on E and (E,‖⋅‖) is a Hilbert space (see [1,Lemma 7]) with scalar product
(u,v)=∫R2N[u(x)−u(y)][v(x)−v(y)]K(x−y)dxdy. |
Note that C∞c(Ω) is dense in E and the norm ‖⋅‖ involves the interaction between Ω and RN∖Ω.
The weak formulation of problem (1.1) and (1.3) is given by
∫R2N[u(x)−u(y)][v(x)−v(y)]K(x−y)dxdy=λ1∫Ωu(x)v(x)dx+∫Ωf(x,u)vdx, ∀ v∈X, |
and
∫R2N[u(x)−u(y)][v(x)−v(y)]|x−y|N+2sdxdy=λ1∫Ωu(x)v(x)dx+∫Ωf(x,u)vdx, ∀ v∈X, |
which represents the Euler-Lagrange equation of the functional I,I0:X→R defined as
I(u):=12∫R2N|u(x)−u(y)|2K(x−y)dxdy−λ12∫Ω|u(x)|2dx−∫ΩF(x,u)dx, |
and
I0(u):=12∫R2N|u(x)−u(y)|2|x−y|N+2sdxdy−λ12∫Ω|u(x)|2dx−∫ΩF(x,u)dx. |
To give our result, first we recall the eigenvalues of the following problem
{−LKu=λuin Ω,u=0in RN∖Ω. | (1.4) |
Proposition 1.1. [12,23] Let s∈(0,1), N>2s, Ω be an open, bounded subset of RN, and let K:RN∖{0}→(0,+∞) be a function satisfying assumptions (K1) and (K2). Then
(a) problem (1.4) admits a eigenvalue λ1 that is a positive and that can be characterized as follows:
λ1=minu∈E∖{0}∫R2N|u(x)−u(y)|2K(x−y)dxdy∫Ω|u(x)|2dx; |
(b) there exists a nonnegative function φ1∈E that is an eigenfunction corresponding to λ1, that is, |φ1|2=1 and
λ1=∫R2N|φ1(x)−φ1(y)|2K(x−y)dxdy; |
(c) λ1 is simple, that is, if u∈E is a solution of (1.4) with λ=λ1, then u=ζφ1 for ζ∈R;
(d) the set of the eigenvalues of problem (1.4) consists of a sequence {λk}k∈N with
0<λ1<λ2<λ2<⋯<λk<⋯→∞. |
Remark 1.1. [12] For the fractional Laplacian (−Δ)s, the first eigenfunction φ1 is strictly positive in Ω.
Motivated by the results mentioned above, the main aim of this paper is to establish the existence of multiple non-trivial solutions for (1.1) and (1.3). To the best of authors' knowledge, the existence of multiple solutions for the problem (1.1) and (1.3) has not been well studied. The proof of our results borrow the ideas from [28] in which existence results of positive solutions are obtained for a class of Dirichlet problem. We assume that f(x,t) is a Carathéodory function on Ω×R and satisfies
(f1) |f(x,t)|≤γ|t|, x∈Ω, t∈R, where γ<(λ122−λ121)λ121 and λ1,λ2 are the first two eigenvalues of problem (1.4).
(f2) τ±(x):=lim supt→±∞2F(x,t)t2≤0(≢0), x∈Ω, where F(x,u)=∫u0f(x,s)ds.
(f3) there are constants r1>0 and r2<0 such that ∫ΩF(x,rjφ1)dx>0 (j=1,2), where φ1 is the eigenfunction of problem (1.4) corresponding to λ1.
Our main result can be stated as follow.
Theorem 1.1. Let s∈(0,1), N>2s and Ω be an open bounded set of RN with Lipschitz boundary, assume that K(x) satisfies (K1)−(K2) and the assumption (f1)-(f3) hold with
∫Ω(τ+(x)(φ+1)2+τ−(x)(φ−1)2)dx≤0, | (1.5) |
or
∫Ω(τ+(x)(φ−1)2+τ−(x)(φ+1)2)dx≤0, | (1.6) |
then the problem (1.1) possesses at least two non-trivial solution u1 and u2, one satisfying (u1,φ1)>0 and the other satisfying (u2,φ1)<0.
In the non-local framework, the simplest example we can deal with is given by the fractional Laplacian (−Δ)s, according to the following result:
Theorem 1.2. Let s∈(0,1), N>2s and Ω be an open bounded set of RN with Lipschitz boundary, assume that the assumption (f1)-(f3) hold, then the problem (1.5) possesses at least two non-trivial solution u1 and u2, one satisfying (u1,φ1)>0 and the other satisfying (u2,φ1)<0.
The paper is organized as follows. In the forthcoming Section 2, we collect some necessary preliminary observations and devote ourselves to the proof of Theorems. Final, we give some conclusions in Section 3. Through the paper, we make use of following notations: C,C0,C1,⋅⋅⋅ for positive constants (possibly different from line to line).
Our results are based upon the following critical point theorems in Hilbert space.
Proposition 2.1. ([28]) Let G∈C1(E) for some Hilbert space E and is bounded on bounded sets. Assume that there exist constants θ<1, d∈R, u0∈E and a unit vector φ0∈E such that
(u0,φ0)≤d | (2.1) |
and
(G′(u),φ0)≤θ‖G′(u)‖ where (u,φ0)=d and G(u)≥G(u0). | (2.2) |
Assume also that there is a β≥1 satisfying
lim supR→∞R−βsup{G(u):‖u‖=R,(u,φ0)≤d}≤0. | (2.3) |
Then there is a sequence {uk}⊂E such that
(uk,φ0)≤d, G(uk)→c, G(u0)≤c≤∞, ‖G′(uk)‖=o(‖uk‖β−1+1). | (2.4) |
In addition, if (2.1)−(2.3) are replaced by
(u0,φ0)≥d, | (2.5) |
(G′(u),φ0)+θ‖G′(u)‖≥0 where (u,φ0)=d and G(u)≥G(u0) | (2.6) |
and
lim supR→∞R−βsup{G(u):‖u‖=R,(u,φ0)≥d}≤0, | (2.7) |
respectively. Then there is a sequence {uk}⊂E satisfying
(uk,φ0)≥d, G(uk)→c, G(u0)≤c≤∞, ‖G′(uk)‖=o(‖uk‖β−1+1). | (2.8) |
Remark 2.1. Note that the condition (2.2) allows us to restrict our attention to the region (u,φ1)≤d, and (2.3) can help us dispense with the requirement that we find two subsets A,B of E such that A links B and supAG≤infBG. Conditions (2.6) and (2.7) are similar. Moreover, this results can allow us to consider problems in which the maximum principle and sub-super solutions do not apply.
Lemma 2.1. Suppose (f1) and in addition that
∫Ω(τ+(x)(u+)2+τ−(x)(u−)2)dx≤0, (u,φ1)≥0 | (2.9) |
and
∫Ω(τ+(x)(φ+1)2+τ−(x)(φ−1)2)dx<0, | (2.10) |
where τ± is defined as (f2). Assume also that
∫ΩF(x,rφ1)dx>0 | (2.11) |
for some r>0. Then there is at least one non-trivial solution of problem (1.1) satisfying (u,φ1)>0.
In addition, if we replace (2.9), (2.10) and (2.11) by
∫Ω(τ+(x)(u+)2+τ−(x)(u−)2)dx≤0, (u,φ1)≤0, | (2.12) |
∫Ω(τ+(x)(φ−1)2+τ−(x)(φ+1)2)dx<0 | (2.13) |
and
∫ΩF(x,−rφ1)dx>0, | (2.14) |
then there is another solution satisfying (u,φ1)<0.
Proof. We only prove the first conclusion, the other is similar. Let
J(u)=−‖u‖2+λ1|u|22+2∫ΩF(x,u)dx, |
and take u0=rφ1,d=0,β=2 in Proposition 2. We first verify (2.7), suppose on the contrary that there is a sequence {uk}⊂E such that (uk,φ1)≥0,ρk=‖uk‖→∞ and
J(uk)ρ2k≥c>0, k=1,2,⋯. | (2.15) |
Let ˜uk=ukρk. Then we have that (˜uk,φ1)≥0, ‖˜uk‖=1, and there exists a subsequence such that ˜uk⇀˜u in E and a.e. in Ω. Therefore
lim supk→∞J(uk)ρ2k≤2∫Ωlim supk→∞F(x,uk)u2k˜u2kdx≤∫Ω(τ+(˜u+)2+τ−(˜u−)2)dx≤0, |
which is a contradiction with (2.15). Next we claim that (2.6) holds. Note that from (f1), for any u⊥φ1 we have
|(J′(u)),φ1|=2|(f(x,u),φ1)|≤2|f(x,u)|2|φ1|2≤2γ‖u‖(λ1λ2)12, |
where we take λ1|φ1|22=‖φ1‖2=1 and λ2|u|22≤‖u‖2 for u⊥φ1. Therefore, for any u⊥φ1 we have
|(J′(u),φ1)|≤θ‖J′(u)‖, |
where θ=γ(λ1λ2)1211−λ1+γλ2<1. So (2.6) holds and it follows from Proposition 2 that there exists a sequence satisfying (2.8). Assume ρk=‖uk‖→∞ and let ˜uk=ukρk. Then we have a subsequence converging weakly to a function ˜u in E and a.e. in Ω. Since
J(uk)ρ2k=2∫ΩF(x,uk)ρ2kdx+λ1|˜uk|22−1, |
we can know that
0≤∫Ω(τ+(˜u+)2+τ−(˜u−)2)dx+λ1|˜u|22−1≤λ1|˜u|22−‖u‖2≤0. |
Therefore,
∫Ω(τ+(˜u+)2+τ−(˜u−)2)dx=0 | (2.16) |
and
‖˜u‖2=λ1|˜u|22=1. | (2.17) |
Because λ1 is a simple eigenvalue of −Lk and (˜u,φ1)≥0, it follows from (2.17) that ˜u=φ1. So (2.16) reduces to
∫Ω(τ+(φ+1)2+τ−(φ−1)2)dx=0, |
which is a contradiction with (2.10). In consequence, ρk are bounded and standard methods show that there is a subsequence of {uk} converging in E to a solution satisfying
(u,φ1)≥0, J(u)=c, J(u0)≤c, J′(u)=0. |
Finally, we verify that (u,φ1)>0. If (u,φ1)=0, then
(λ2−λ1)|u|22≤‖u‖2−λ1|u|22=(f(x,u),u)≤γ|u|22. |
But γ<λ2−λ1, which is a contradiction. We only replace φ1 by −φ1 in the above proof, the second conclusion is proved. Therefore, the proof of Lemma 2.1 is complete.
It follows from (f2) that
τ±(x)≤0, x∈Ω, |
then we have (2.9) and (2.12) hold. Therefore, the hypotheses of Lemma 2.1 are satisfied. Then, it follows from Lemma 2.1 that problem (1.1) has at least two non-trivial solution, one satisfying (u,φ1)>0 and the other one satisfying (u,φ1)<0. Therefore, the proof of Theorem 1.1 is complete.
Note that φ1>0 a.e. in Ω, then we can replace (2.10) with
τ+(x)≤0, τ+(x)≢0, |
and (2.13) with
τ−(x)≤0, τ−(x)≢0. |
Then Theorem 1.2 follows from Theorem 1.1.
In this paper, we generalize critical point theory to the nonlocal problem in which general methods such as maximum principle and sub-super solutions can not be applied. We can distinguish between different solutions via showing that they are located in different parts of the Hilbert space. Several recent results of the literatures are extended and improved.
We would like to thank the anonymous referee for his/her careful readings of our manuscript and the useful comments made for its improvement. This work is supported by National Natural Science Foundation of China (No.11861078, 11771385).
The authors declare no conflict of interest.
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