Normalized solutions to the Schrödinger systems with double critical growth and weakly attractive potentials

In this paper, we look for solutions to the following critical Schrödinger system { − Δ u + ( V 1 + λ 1 ) u = | u | 2 ∗ − 2 u + | u | p 1 − 2 u + β r 1 | u | r 1 − 2 u | v | r 2 i n   R N , − Δ v + ( V 2 + λ 2 ) v = | v | 2 ∗ − 2 v + | v | p 2 − 2 v + β r 2 | u | r 1 | v | r 2 − 2 v i n   R N , havi...

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Published inElectronic journal of qualitative theory of differential equations Vol. 2023; no. 42; pp. 1 - 22
Main Authors Long, Lei, Feng, Xiaojing
Format Journal Article
LanguageEnglish
Published University of Szeged 01.01.2023
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Abstract In this paper, we look for solutions to the following critical Schrödinger system { − Δ u + ( V 1 + λ 1 ) u = | u | 2 ∗ − 2 u + | u | p 1 − 2 u + β r 1 | u | r 1 − 2 u | v | r 2 i n   R N , − Δ v + ( V 2 + λ 2 ) v = | v | 2 ∗ − 2 v + | v | p 2 − 2 v + β r 2 | u | r 1 | v | r 2 − 2 v i n   R N , having prescribed mass ∫ R N u 2 = a 1 > 0 and ∫ R N v 2 = a 2 > 0 , where λ 1 , λ 2 ∈ R will arise as Lagrange multipliers, N ⩾ 3 , 2 ∗ = 2 N / ( N − 2 ) is the Sobolev critical exponent, r 1 , r 2 > 1 , p 1 , p 2 , r 1 + r 2 ∈ ( 2 + 4 / N , 2 ∗ ) and β > 0 is a coupling constant. Under suitable conditions on the potentials V 1 and V 2 , β ∗ > 0 exists such that the above Schrödinger system admits a positive radial normalized solution when β ⩾ β ∗ . The proof is based on comparison argument and minmax method.
AbstractList In this paper, we look for solutions to the following critical Schrödinger system { − Δ u + ( V 1 + λ 1 ) u = | u | 2 ∗ − 2 u + | u | p 1 − 2 u + β r 1 | u | r 1 − 2 u | v | r 2 i n   R N , − Δ v + ( V 2 + λ 2 ) v = | v | 2 ∗ − 2 v + | v | p 2 − 2 v + β r 2 | u | r 1 | v | r 2 − 2 v i n   R N , having prescribed mass ∫ R N u 2 = a 1 > 0 and ∫ R N v 2 = a 2 > 0 , where λ 1 , λ 2 ∈ R will arise as Lagrange multipliers, N ⩾ 3 , 2 ∗ = 2 N / ( N − 2 ) is the Sobolev critical exponent, r 1 , r 2 > 1 , p 1 , p 2 , r 1 + r 2 ∈ ( 2 + 4 / N , 2 ∗ ) and β > 0 is a coupling constant. Under suitable conditions on the potentials V 1 and V 2 , β ∗ > 0 exists such that the above Schrödinger system admits a positive radial normalized solution when β ⩾ β ∗ . The proof is based on comparison argument and minmax method.
In this paper, we look for solutions to the following critical Schrödinger system $$\begin{cases} -\Delta u+(V_1+\lambda_1)u=|u|^{2^*-2}u+|u|^{p_1-2}u+\beta r_1|u|^{r_1-2}u|v|^{r_2}&{\rm in}\ \mathbb{R}^N,\\ -\Delta v+(V_2+\lambda_2)v=|v|^{2^*-2}v+|v|^{p_2-2}v+\beta r_2|u|^{r_1}|v|^{r_2-2}v&{\rm in}\ \mathbb{R}^N, \end{cases}$$ having prescribed mass $\int_{\mathbb{R}^N}u^2=a_1>0$ and $\int_{\mathbb{R}^N}v^2=a_2>0$, where $\lambda_1,\lambda_2\in\mathbb{R}$ will arise as Lagrange multipliers, $N\geqslant3$, $2^*=2N/(N-2)$ is the Sobolev critical exponent, $r_1,r_2>1$, $p_1,p_2,r_1+r_2\in(2+4/N,2^*)$ and $\beta>0$ is a coupling constant. Under suitable conditions on the potentials $V_1$ and $V_2$, $\beta_*>0$ exists such that the above Schrödinger system admits a positive radial normalized solution when $\beta\geqslant\beta_*$. The proof is based on comparison argument and minmax method.
Author Feng, Xiaojing
Long, Lei
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Snippet In this paper, we look for solutions to the following critical Schrödinger system { − Δ u + ( V 1 + λ 1 ) u = | u | 2 ∗ − 2 u + | u | p 1 − 2 u + β r 1 | u | r...
In this paper, we look for solutions to the following critical Schrödinger system $$\begin{cases} -\Delta u+(V_1+\lambda_1)u=|u|^{2^*-2}u+|u|^{p_1-2}u+\beta...
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positive solutions
schrödinger systems
weakly attractive potentials
Title Normalized solutions to the Schrödinger systems with double critical growth and weakly attractive potentials
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