In this paper, we consider the following Kirchhoff-type equation:
−(a+b∫R3|∇u|2dx)Δu+u=|u|p−1u,inR3,
where a, b>0, p∈(1,5). By considering a minimization problem on a special constraint set, we prove that the above problem has at least one sign-changing solution for any p∈(1,5). Our results (especially p∈(1,3]) can be regarded as an improvement on the existing results.
Citation: Ting Xiao, Yaolan Tang, Qiongfen Zhang. The existence of sign-changing solutions for Schrödinger-Kirchhoff problems in R3[J]. AIMS Mathematics, 2021, 6(7): 6726-6733. doi: 10.3934/math.2021395
[1] | Ya-Lei Li, Da-Bin Wang, Jin-Long Zhang . Sign-changing solutions for a class of p-Laplacian Kirchhoff-type problem with logarithmic nonlinearity. AIMS Mathematics, 2020, 5(3): 2100-2112. doi: 10.3934/math.2020139 |
[2] | Xia Li, Wen Guan, Da-Bin Wang . Least energy sign-changing solutions of Kirchhoff equation on bounded domains. AIMS Mathematics, 2022, 7(5): 8879-8890. doi: 10.3934/math.2022495 |
[3] | Jinfu Yang, Wenmin Li, Wei Guo, Jiafeng Zhang . Existence of infinitely many normalized radial solutions for a class of quasilinear Schrödinger-Poisson equations in $ \mathbb{R}^3 $. AIMS Mathematics, 2022, 7(10): 19292-19305. doi: 10.3934/math.20221059 |
[4] | Qing Yang, Chuanzhi Bai . Sign-changing solutions for a class of fractional Kirchhoff-type problem with logarithmic nonlinearity. AIMS Mathematics, 2021, 6(1): 868-881. doi: 10.3934/math.2021051 |
[5] | Ziqing Yuan, Jing Zhao . Solutions for gauged nonlinear Schrödinger equations on $ {\mathbb R}^2 $ involving sign-changing potentials. AIMS Mathematics, 2024, 9(8): 21337-21355. doi: 10.3934/math.20241036 |
[6] | Ye Xue, Zhiqing Han . Existence and multiplicity of solutions for Schrödinger equations with sublinear nonlinearities. AIMS Mathematics, 2021, 6(6): 5479-5492. doi: 10.3934/math.2021324 |
[7] | Jie Yang, Lintao Liu, Haibo Chen . Multiple positive solutions to the fractional Kirchhoff-type problems involving sign-changing weight functions. AIMS Mathematics, 2024, 9(4): 8353-8370. doi: 10.3934/math.2024406 |
[8] | Zhongxiang Wang, Gao Jia . Existence of solutions for modified Kirchhoff-type equation without the Ambrosetti-Rabinowitz condition. AIMS Mathematics, 2021, 6(5): 4614-4637. doi: 10.3934/math.2021272 |
[9] | Zhongxiang Wang . Existence and asymptotic behavior of normalized solutions for the modified Kirchhoff equations in $ \mathbb{R}^3 $. AIMS Mathematics, 2022, 7(5): 8774-8801. doi: 10.3934/math.2022490 |
[10] | Yuan Shan, Baoqing Liu . Existence and multiplicity of solutions for generalized asymptotically linear Schrödinger-Kirchhoff equations. AIMS Mathematics, 2021, 6(6): 6160-6170. doi: 10.3934/math.2021361 |
In this paper, we consider the following Kirchhoff-type equation:
−(a+b∫R3|∇u|2dx)Δu+u=|u|p−1u,inR3,
where a, b>0, p∈(1,5). By considering a minimization problem on a special constraint set, we prove that the above problem has at least one sign-changing solution for any p∈(1,5). Our results (especially p∈(1,3]) can be regarded as an improvement on the existing results.
In this paper, we study the existence of sign-changing solution to the following Kirchhoff equation by using a direct method
−(a+b∫R3|∇u|2dx)Δu+u=|u|p−1u,inR3, | (1.1) |
where a, b>0, p∈(1,5). In recent years, problem (1.1) has been extensively researched by many mathematicians. Therefore, there are a large number of results for the existence of nontrivial solutions, positive solutions, ground state solutions, sign-changing solutions, nodal solutions for problem (1.1). Please see [1,2,3,4,5,6] and the references therein. It is worth noting that Chen, Fu and Wu [4] established the existence of a positive ground state solution to problem (1.1) for any b>0 and p∈(1,5). However, there is a question: whether problem (1.1) has sign-changing solutions for any p∈(1,5)?
Recently, Wang, Zhang and Cheng [7] established the existence results of sign-changing solutions to the following problem
−(a+b∫R3|∇u|2dx)Δu+V(x)u=f(u),inR3, | (1.2) |
where f(t) satisfies the following crucial conditions:
(f1) limt→∞F(t)t4=∞, where F(t)=∫t0f(s)ds;
(f2) f(t)t3 is nondecreasing for |t|>0.
Obviously, when p∈(1,3], f(t)=|t|p−1t does not satisfy (f1) and (f2). Qian [8] researched the existence of a ground state sign-changing solution to the following problem
{−(a−λ∫Ω|∇u|2dx)Δu=|u|q−2u,inΩ,u=0,on∂Ω, | (1.3) |
where a is a positive constant, q∈(2,2∗)(2∗=+∞ for N=1,2, 2∗=2NN−2 for N≥3), Ω⊂R3 is a bounded domain and λ>0 is a parameter. They mainly obtained that problem (1.3) has at least one sign-changing solution for small enough λ, thanks to truncated technique and constraint variational method. Besides, some similar problems have also been extensively researched. For more relevant results, please refer to [9,10] and the references therein.
Motivated by the above mentioned results, our result is given in the following.
Theorem 1.1 For any a, b>0 and p∈(1,5), problem (1.1) has at least one sign-changing solution.
Remark 1.2 When p∈(3,5), the existence of one sign-changing solution to (1.1) is obtained by [7]. But when p∈(1,3], it is difficult to prove the existence of sign-changing solutions. The main difficulty lies in proving the functional of problem (1.1) satisfies (PS)-conditions. To overcome this difficulty, we will apply some new tricks. Moreover, f(t)≜|t|p−1t does not satisfy (f1)-(f2) when p∈(1,3]. We must point out that our result holds for any b>0. Therefore, our result can be seen as an improvement and extension of [7,8]. Our result can also extent to more general f(u).
In this paper, we shall work on the space
E=H1r(R3)≜{u∈H1(R3):u(|x|)=u(x)} |
with the inner product and norm
⟨u,v⟩=∫R3(a∇u∇v+uv)dx,‖u‖=⟨u,u⟩12. |
Lq(R3)(1≤q<∞) denotes Lebesgue space with norm ‖u‖q=(∫R3|u|qdx)1/q. It is well known that the weak solution of problem (1.1) corresponds to the critical point of
I(u)=12∫R3(a|∇u|2dx+|u|2)dx+b4(∫R3|∇u|2dx)2−1p+1∫R3|u|p+1dx. | (1.4) |
Clearly, I∈C1(E,R) and we have
⟨I′(u),v⟩=∫R3(a∇u∇v+uv)dx+b∫R3|∇u|2dx∫R3∇u∇vdx−∫R3|u|p−1uvdx. | (1.5) |
Setting u+=max{u,0}, u−=min{u,0}, A(u+,u−)=b2∫R3|∇u+|2dx∫R3|∇u−|2dx. To state our result, we establish the following minimization problem
c≜inf{I(u):u∈M}, | (1.6) |
where
M≜{u∈E:u±≠0,12⟨I′(u),u+⟩+P(u+)+A(u+,u−)=12⟨I′(u),u−⟩+P(u−)+A(u+,u−)=0}, | (1.7) |
P(u)=a2∫R3|∇u|2dx+32∫R3|u|2dx+b2(∫R3|∇u|2dx)2−3p+1∫R3|u|p+1dx. |
Obviously, the set M is a subset of the following special manifold:
N≜{u∈E:12⟨I′(u),u⟩+P(u)=0}. | (1.8) |
Remark 1.3 Clearly, the manifold M has not been used in the existing literature. The usual manifold M1 has been used in previous literature is a subset of manifold N1, where
M1={u∈E:u±≠0,⟨I′(u),u+⟩=⟨I′(u),u−⟩=0},N1={u∈E:⟨I′(u),u⟩=0}. |
As we all know, the manifold N1 is a commonly used manifold in the study of positive solutions. But the manifold M1 is not enough for us to prove our result when p∈(1,3]. Thus, we need to find an another manifold. For researching positive solutions, one can also use a special manifold N, which is a combination of the Nehari manifold and Pohožaev manifold for power p∈(1,5). In order to prove our result, we choose the manifold M.
Comparing with the 4-superlinear condition in [7], we meet some new difficulties. We need to show that the constraint set M is nonempty and the minimizing sequence on M is a (PS)-sequence of I in E by using some new tricks.
Lemma 2.1 If p∈(1,5), then M≠∅.
Proof. For any u∈E and u±≠0, we set ut≜t12u(xt). In the following, we shall prove that there are positive constants s1 and t1 such that
12⟨I′(u+s1+u−t1),u+s1⟩+P(u+s1)+A(u+s1,u−t1)=12⟨I′(u+s1+u−t1),u−t1⟩+P(u−t1)+A(u+s1,u−t1)=0, | (2.1) |
which implies that u+s1+u−t1∈M. Actually, equation (2.1) holds if and only if
{r(s,t)≜as2α(u+)+s4[2β(u+)+bγ(u+)]+2s2t2A(u+,u−)−p+72(p+1)sp+72ξ(u+)=0,l(s,t)≜at2α(u−)+t4[2β(u−)+bγ(u−)]+2s2t2A(u+,u−)−p+72(p+1)tp+72ξ(u−)=0, | (2.2) |
where
α(u)≜∫R3|∇u|2dx, β(u)≜∫R3|u|2dx, γ(u)≜(∫R3|∇u|2dx)2, ξ(u)≜∫R3|u|p+1dx. | (2.3) |
In the other words, we only need to show that there exists m∈(0,M) such that
r(m,t)>0,r(M,t)<0,∀ t∈[m,M], | (2.4) |
l(s,m)>0,l(s,M)<0,∀ s∈[m,M], | (2.5) |
where M is a positive constant. Since p∈(1,5), then p+72>4. By (2.2), we can derive that r(s,t)<0 as s enough large, r(s,t)>0 as s enough small. And l(s,t)<0 as t enough large, l(s,t)>0 as t enough small. Consequently, (2.4)-(2.5) hold. Then from the Miranda's Theorem [11], there exist two positive constants s1 and t1 such that
r(s1,t1)=0,l(s1,t1)=0. | (2.6) |
Hence, (2.1) holds, which shows that u+s1+u−t1∈M, i.e., M≠∅. The proof is completed.
Lemma 2.2 The pair (s1,t1) with positive numbers in Lemma 2.1 is unique.
Proof. In view of Lemma 2.1, there exists a pair (s1,t1) such that u+s1+u−t1∈M for any u∈E and u±≠0. Next, we shall prove the uniqueness of (s1,t1) by two steps.
Step 1. If u∈M, then (s1,t1)=(1,1).
Since u∈M, then we have
{r(1,1)≜aα(u+)+2β(u+)+bγ(u+)+2A(u+,u−)−p+72(p+1)ξ(u+)=0,l(1,1)≜aα(u−)+2β(u−)+bγ(u−)+2A(u+,u−)−p+72(p+1)ξ(u−)=0. | (2.7) |
Assume that s1≤t1. By (2.2), we have
1s21aα(u+)+2β(u+)+bγ(u+)+2A(u+,u−)≤p+72(p+1)sp−121ξ(u+), | (2.8) |
1t21aα(u−)+2β(u−)+bγ(u−)+2A(u+,u−)≥p+72(p+1)tp−121ξ(u−). | (2.9) |
It follows from (2.7) and (2.8) that
(1s21−1)a∫R3|∇u+|2dx≤p+72(p+1)[sp−121−1]∫R3|u+|p+1dx. | (2.10) |
If s1<1, the negative right side of inequality (2.10) contradicts the positive left side. So 1≤s1≤t1. Moveover, combining (2.7) and (2.9), t1≤1 can be also obtained. Then (s1,t1)=(1,1).
Step 2. If u∉M, then there exists a unique u1 such that u+1+u−1∈M.
Suppose that there is an another pair (s2,t2) such that u+s2+u−t2∈M. We set v1≜u+s1+u−t1 and v2≜u+s2+u−t2. By a simple calculation, we have
∫R3[s7/22s7/21v+1+t7/22t7/21v−1]dx=s7/22∫R3u+dx+t7/22∫R3u−dx=∫R3(v+2+v−2)dx. | (2.11) |
Thanks to v2∈M and step 1, we deduce that (s1,t1)=(s2,t2). The proof is completed.
Similar to [7], we can prove that I(u+s1+u−t1)=maxs,t≥0I(u+s+u−t). From Lemma 2.2, we consider the minimization problem
cM≜inf{I(u):u∈M}. | (2.12) |
Lemma 2.3 cM is achieved.
Proof. For each u∈M, we have G(u)≜12⟨I′(u),u⟩+P(u)=0. Then for any p∈(1,5), we have
I(u)=I(u)−14G(u)=14a∫R3|∇u|2dx+p−18(p+1)∫R3|u|p+1dx≥14a∫R3|∇u|2dx>0. | (2.13) |
That is cM>0. Letting {un}⊂M such that I(un)→cM. From (2.13), we know that {|∇un|2} is bounded in E. Since G(un)=0, then
2∫R3|un|2dx=p+72(p+1)∫R3|un|p+1dx−a∫R3|∇un|2dx−b(∫R3|∇un|2dx)2≤p+72(p+1)‖un‖p+1p+1. | (2.14) |
From Hölder and Sobolev inequalities, we have
‖un‖p+1p+1≤‖un‖(p+1)ϑ2‖un‖(p+1)(1−ϑ)6≤C‖un‖(p+1)ϑ2‖∇un‖(p+1)(1−ϑ)2, | (2.15) |
where 1p+1=ϑ2+1−ϑ6. Then (p+1)ϑ<2. According to Young's inequality, we obtain that for any ε>0, there exists Cε>0 such that
p+72(p+1)‖un‖p+1p+1≤ε‖un‖22+Cε‖∇un‖2(p+1)(1−ϑ)2−(p+1)ϑ2. | (2.16) |
Set ε=1, from (2.14) and (2.16), we have that {‖un‖2} is bounded. Hence, {un} is bounded. Then, there exists u such that u±n⇀u± in E. From (2.13), we can find a constant θ such that ‖u±n‖>θ>0 for every n∈N.
Since {un}⊂M, we have that
a∫R3|∇u±n|2dx+2∫R3|u±n|2dx+b∫R3|∇un|2dx∫R3|∇u±n|2dx=p+72(p+1)∫R3|u±n|p+1dx. | (2.17) |
Therefore, we have
θ2≤‖u±n‖2<C1∫R3|u±n|p+1dx. | (2.18) |
Then ∫R3|u±n|p+1dx>θ2C1>0. Since the embedding E↪Lq(R3) is compact for 2<q<6, (2.18) shows that u±≠0. Combining the compactness lemma of Strauss [11] and the weak semicontinuity of norm, we obtain
limn→∞∫R3|u±n|p+1dx→∫R3|u±|p+1dx, | (2.19) |
a∫R3|∇u±|2dx+2∫R3|u±|2dx≤lim infn→∞(a∫R3|∇u±n|2dx+2∫R3|u±n|2dx) | (2.20) |
and
b∫R3|∇u|2dx∫R3|∇u±|2dx≤lim infn→∞b∫R3|∇un|2dx∫R3|∇u±n|2dx. | (2.21) |
Then from (2.17) and (2.19)–(2.21), we have that
12⟨I′(u),u±⟩+p(u±)+A(u++u−)≤lim infn→∞{12⟨I′(un),u±n⟩+p(u±n)+A(u+n+u−n)}=0. | (2.22) |
Thus, there exists (su,tu) such that u+su+u−tu∈M. Suppose that 0<tu≤su, then we obtain
as2u∫R3|∇u+|2dx+2s4u∫R3|u+|2dx+bs4u(∫R3|∇u+|2dx)2+bs4u∫R3|∇u+|2dx∫R3|∇u−|2dx≥s2u∫R3|∇u+|2dx+2s4u∫R3|u+|2dx+bs4u(∫R3|∇u+|2dx)2+bs2ut2u∫R3|∇u+|2dx∫R3|∇u−|2dx=p+72(p+1)sp+72u∫R3|u+|p+1dx. | (2.23) |
From (2.19) and (2.22), we have
a∫R3|∇u+|2dx+2∫R3|u+|2dx+b∫R3|∇u|2dx∫R3|∇u+|2dx≤p+72(p+1)∫R3|u+|p+1dx. | (2.24) |
By (2.23) and (2.24), we obtain
a(1s2u−1)∫R3|∇u+|2dx≥p+72(p+1)(sp−12u−1)∫R3|u+|p+1dx, |
which shows su≤1. Then 0<tu≤su≤1. Setting ˉu=u+su+u−tu. Therefore, we can deduce that
cM≤I(ˉu)−14G(ˉu)=14as2u∫R3|∇u+|2dx+p−18(p+1)sp+72u∫R3|u+|p+1dx+14at2u∫R3|∇u−|2dx+p−18(p+1)tp+72u∫R3|u−|p+1dx≤14a∫R3|∇u+|2dx+p−18(p+1)∫R3|u+|p+1dx+14a∫R3|∇u−|2dx+p−18(p+1)∫R3|u−|p+1dx=I(u)−14G(u)≤lim infn→∞(I(un)−14G(un))=cM. | (2.25) |
(2.25) implies that su=tu=1. That is u=ˉu and I(u)=cM. The proof is completed.
Lemma 3.1. Assume cM attained in M, then u is a critical point of I.
Proof. Since u∈M, u±≠0. Then for any fixed v∈H1(R3), there exists ε>0 such that (u+wv)±≠0 for all w∈(−ε,ε). Arguing by a contradiction, there is a sequence {wi}∞i=1 such that
limi→∞wi=0,u+wiv=0 a.e. on R3. |
Letting i→∞, we have u=0 a.e. on R3. Which is a contradiction with u±≠0.
From Lemma 2.1, there exists a unique pair (s(w),t(w)) such that s(w)(u+wv)++t(w)(u+wv)−∈M. Next, we prove some standard properties of (s(w),t(w)) as Nehari manifold. For our purpose, we consider the function
φ(s,t,w)=G((u+wv)+s+(u+wv)−t) |
defined for (s,t,w)∈(0,+∞)×(0,+∞)×(−ε,ε). Since u∈M, we have φ(1,1,0)=0. Moveover, φ is a C1 function and
∂φ(s,t,w)∂s|(s,t,w)=(1,1,0)=−p2+6p−74(p+1)∫R3|u+|p+1dx−2a∫R3|∇u+|2dx≤0. |
Similarly, we can deduce that ∂φ(s,t,w)∂t|(s,t,w)=(1,1,0)≤0. From the Implicit Function Theorem, the functions s(w), t(w) are C1. And t(0)=s(0)=1. Moveover, s(w), t(w)≠0 near 0. We define
Υ(w)=I((u+wv)+s(w)+(u+wv)−t(w)). |
Then we obtain that Υ is differentiable for small w and attains its minimum at w=0. Hence, we derive that
0=Υ′(0)=dI((u+wv)+s(w)+(u+wv)−t(w))dw|w=0=∂I((u+wv)+s(w)+(u+wv)−t(w))∂s|(s,t,w)=(1,1,0)dsdw|w=0+dI((u+wv)+s(w)+(u+wv)−t(w))dw|(s,t,w)=(1,1,0)+∂I((u+wv)+s(w)+(u+wv)−t(w))∂t|(s,t,w)=(1,1,0)dtdw|w=0=r(1,1)s′(0)+l(1,1)t′(0)+⟨I′(u),v⟩=⟨I′(u),v⟩. |
Since v∈E is arbitrary, we have that I′(u)=0.
Proof of Theorem 1.1. From Lemma 2.3 and 3.1, there is a u∈M such that I(u)=cM and I′(u)=0. Then problem (1.1) has at least one sign-changing solution. The proof is completed.
The authors would like to thank the editors and referees for their useful suggestions which have significantly improved the paper. This work is supported by the National Natural Science Foundation of China (No. 11961014, No. 61563013) and Guangxi Natural Science Foundation (2016GXNSFAA380082, 2018GXNSFAA281021).
The authors declare that they have no competing interests.
[1] |
J. Sun, S. B. Liu, Nontrivial solutions of Kirchhoff type problems, Appl. Math. Lett., 25 (2012), 500–504. doi: 10.1016/j.aml.2011.09.045
![]() |
[2] |
Z. J. Guo, Ground states for Kirchhoff equations without compact condition, J. Differ. Equations, 259 (2015), 2884–2902. doi: 10.1016/j.jde.2015.04.005
![]() |
[3] |
Q. Q. Li, K. M. Teng, X. Wu, Ground states for Kirchhoff-type equations with critical or supercritical growth, Math. Method. Appl. Sci., 40 (2017), 6732–6746. doi: 10.1002/mma.4485
![]() |
[4] |
W. Chen, Z. W. Fu, Y. Wu, Positive solutions for nonlinear Schrödinger-Kirchhoff equations in R3, Appl. Math. Lett., 104 (2020), 106274. doi: 10.1016/j.aml.2020.106274
![]() |
[5] |
Q. L. Xie, Least energy nodal solution for Kirchhoff type problem with an asymptotically 4-linear nonlinearity, Appl. Math. Lett., 102 (2020), 106157. doi: 10.1016/j.aml.2019.106157
![]() |
[6] |
G. B. Li, H. Y. Ye, Existence of positive ground state solutions for the nonlinear Kirchhoff type equations in R3, J. Differ. Equations, 257 (2014), 566–600. doi: 10.1016/j.jde.2014.04.011
![]() |
[7] |
L. Wang, B. L. Zhang, K. Cheng K, Ground state sign-changing solutions for the Schödinger-Kirchhoff equation in R3, J. Math. Anal. Appl., 466 (2018), 1545–1569. doi: 10.1016/j.jmaa.2018.06.071
![]() |
[8] | X. T. Qian, Ground state sign-changing solutions for a class of nonlocal problem, J. Math. Anal. Appl., 2 (2021), 124753. |
[9] | S. T. Chen, Y. B. Li, X. H. Tang, Sign-changing solutions for asymptotically linear Schrödinger equation in bounded domains, Electron. J. Differ. Eq., 317 (2016), 1–9. |
[10] |
G. Q. Chai, W. M. Liu, Least energy sign-changing solutions for Kirchhoff-Poisson systems, Bound. Value Probl., 2019 (2019), 1–25. doi: 10.1186/s13661-018-1115-7
![]() |
[11] | G. Kirchhoff, Mechanik, Teubner, Leipzig, 1883. |
1. | Cuiling Liu, Xingyong Zhang, Existence and multiplicity of solutions for a quasilinear system with locally superlinear condition, 2023, 12, 2191-950X, 10.1515/anona-2022-0289 | |
2. | Noufe H. Aljahdaly, Nouf A. Almushaity, A diffusive cancer model with virotherapy: Studying the immune response and its analytical simulation, 2023, 8, 2473-6988, 10905, 10.3934/math.2023553 | |
3. | Sami Baraket, Rima Chetouane, Rached Jaidane, Wafa Mtaouaa, Sign-changing solutions for a weighted Schrödinger–Kirchhoff equation with double exponential nonlinearities growth, 2024, 36, 0129-055X, 10.1142/S0129055X24500041 | |
4. | Rima Chetouane, Rached Jaidane, Sign-changing solutions for Kirchhoff weighted equations under double exponential nonlinearities growth, 2023, 133, 0973-7685, 10.1007/s12044-023-00760-4 | |
5. | Brahim Dridi, Rached Jaidane, Rima Chetouane, Existence of Signed and Sign-Changing Solutions for Weighted Kirchhoff Problems with Critical Exponential Growth, 2023, 188, 0167-8019, 10.1007/s10440-023-00616-z | |
6. | Brahim Dridi, Abir Amor Ben Ali, Rached Jaidane, Sign-changing solutions for a weighted Kirchhoff problem with exponential growth non-linearity, 2024, 1747-6933, 1, 10.1080/17476933.2024.2310250 | |
7. | Sami Baraket, Rima Chetouane, Rached Jaidane, Signed and Sign-Changing Solutions for a Kirchhoff-Type Problem Involving the Weighted N-Laplacian with Critical Double Exponential Growth, 2023, 2305-221X, 10.1007/s10013-023-00667-7 |