WEAK POTENTIAL CONDITIONS FOR SCHRÖDINGER EQUATIONS WITH CRITICAL NONLINEARITIES

2015 ◽  
Vol 100 (2) ◽  
pp. 272-288
Author(s):  
X. H. TANG ◽  
SITONG CHEN

In this paper, we prove the existence of nontrivial solutions to the following Schrödinger equation with critical Sobolev exponent: $$\begin{eqnarray}\left\{\begin{array}{@{}l@{}}-{\rm\Delta}u+V(x)u=K(x)|u|^{2^{\ast }-2}u+f(x,u),\quad x\in \mathbb{R}^{N},\\ u\in H^{1}(\mathbb{R}^{N})\end{array}\right.\end{eqnarray}$$ under assumptions that (i) $V(x_{0})<0$ for some $x_{0}\in \mathbb{R}^{N}$ and (ii) there exists $b>0$ such that the set ${\mathcal{V}}_{b}:=\{x\in \mathbb{R}^{N}:V(x)<b\}$ has finite measure, in addition to some common assumptions on $K$ and $f$, where $N\geq 3$, $2^{\ast }=2N/(N-2)$.

2021 ◽  
pp. 1-19
Author(s):  
Jing Zhang ◽  
Lin Li

In this paper, we consider the following Schrödinger equation (0.1) − Δ u − μ u | x | 2 + V ( x ) u = K ( x ) | u | 2 ∗ − 2 u + f ( x , u ) , x ∈ R N , u ∈ H 1 ( R N ) , where N ⩾ 4, 0 ⩽ μ < μ ‾, μ ‾ = ( N − 2 ) 2 4 , V is periodic in x, K and f are asymptotically periodic in x, we take advantage of the generalized Nehari manifold approach developed by Szulkin and Weth to look for the ground state solution of (0.1).


2021 ◽  
Vol 21 (2) ◽  
pp. 421-445
Author(s):  
Yuxia Guo ◽  
Ting Liu

Abstract We consider the following nonlinear Schrödinger equation involving supercritical growth: { - Δ ⁢ u + V ⁢ ( y ) ⁢ u = Q ⁢ ( y ) ⁢ u 2 * - 1 + ε in  ⁢ ℝ N , u > 0 , u ∈ H 1 ⁢ ( ℝ N ) , \left\{\begin{aligned} &\displaystyle{-}\Delta u+V(y)u=Q(y)u^{2^{*}-1+% \varepsilon}&&\displaystyle\phantom{}\text{in }\mathbb{R}^{N},\\ &\displaystyle u>0,\quad u\in H^{1}(\mathbb{R}^{N}),\end{aligned}\right.{} where 2 * = 2 ⁢ N N - 2 {2^{*}=\frac{2N}{N-2}} is the critical Sobolev exponent, N ≥ 5 {N\geq 5} , and V ⁢ ( y ) {V(y)} and Q ⁢ ( y ) {Q(y)} are bounded nonnegative functions in ℝ N {\mathbb{R}^{N}} . By using the finite reduction argument and local Pohozaev-type identities, under some suitable assumptions on the functions V and Q, we prove that for ε > 0 {\varepsilon>0} is small enough, problem ( * ) {(*)} has large number of bubble solutions whose functional energy is in the order ε - N - 4 ( N - 2 ) 2 . {\varepsilon^{-\frac{N-4}{(N-2)^{2}}}.}


2014 ◽  
Vol 2014 ◽  
pp. 1-10 ◽  
Author(s):  
Shaowei Chen ◽  
Dawei Zhang

We study the Schrödinger equation:-Δu+Vxu+fx,u=0,  u∈H1(RN), whereVis1-periodic andfis1-periodic in thex-variables;0is in a gap of the spectrum of the operator-Δ+V. We prove that, under some new assumptions forf, this equation has a nontrivial solution. Our assumptions for the nonlinearityfare very weak and greatly different from the known assumptions in the literature.


2019 ◽  
Vol 150 (4) ◽  
pp. 1915-1936 ◽  
Author(s):  
Pietro d'Avenia ◽  
Alessio Pomponio ◽  
Tatsuya Watanabe

AbstractWe are interested in standing waves of a modified Schrödinger equation coupled with the Chern–Simons gauge theory. By applying a constraint minimization of Nehari-Pohozaev type, we prove the existence of radial ground state solutions. We also investigate the nonexistence for nontrivial solutions.


2021 ◽  
Vol 2021 (1) ◽  
Author(s):  
Yan Meng ◽  
Xianjiu Huang ◽  
Jianhua Chen

AbstractIn this paper, we study the following quasilinear Schrödinger equation: $$ -\operatorname{div}\bigl(a(x,\nabla u)\bigr)+V(x) \vert x \vert ^{-\alpha p^{*}} \vert u \vert ^{p-2}u=K(x) \vert x \vert ^{- \alpha p^{*}}f(x,u) \quad \text{in } \mathbb{R}^{N}, $$ − div ( a ( x , ∇ u ) ) + V ( x ) | x | − α p ∗ | u | p − 2 u = K ( x ) | x | − α p ∗ f ( x , u ) in  R N , where $N\geq 3$ N ≥ 3 , $1< p< N$ 1 < p < N , $-\infty <\alpha <\frac{N-p}{p}$ − ∞ < α < N − p p , $\alpha \leq e\leq \alpha +1$ α ≤ e ≤ α + 1 , $d=1+\alpha -e$ d = 1 + α − e , $p^{*}:=p^{*}(\alpha ,e)=\frac{Np}{N-dp}$ p ∗ : = p ∗ ( α , e ) = N p N − d p (critical Hardy–Sobolev exponent), V and K are nonnegative potentials, the function a satisfies suitable assumptions, and f is superlinear, which is weaker than the Ambrosetti–Rabinowitz-type condition. By using variational methods we obtain that the quasilinear Schrödinger equation has infinitely many nontrivial solutions.


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