Normalized solutions to subcritical Choquard systems with double couplings
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arXiv
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| Autori principali: | , |
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| Natura: | Preprint |
| Pubblicazione: |
2025
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| _version_ | 1866917092047978496 |
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| author | Pei, Wenliang Deng, Chonghao |
| author_facet | Pei, Wenliang Deng, Chonghao |
| contents | We consider the Choquard system with both linear and nonlinear couplings
$-Δu + μ_1 u =λ_1 ( I_α* |u|^{r_1} ) |u|^{r_1-2} u + βp( I_α* |v|^q)|u|^{p-2} u + κv,$
$-Δv + μ_2 v =λ_2 ( I_α* |v|^{r_2} ) |v|^{r_2-2} v + βq( I_α* |u|^p)|v|^{q-2} v + κu , $
$\int_{\mathbb{R}^N} u^2 = ρ_1^2\, , \int_{\mathbb{R}^N} v^2 = ρ_2^2,$ where $N \in \{3,4\}$, $λ_1, λ_2, β, κ, ρ_1,ρ_2 > 0$, $2_{α,*} :=\frac{N+α}{N} <p,q , r_1, r_2 <2_α^*:=\frac{N+α}{N-2}$ and $p+q\leq 2r_1 \leq 2r_2$ . We investigate a classification result as the parameters $p+q$, $2r_1$ and $2r_2$ vary across the ranges $(\frac{2N+2α}{N},\frac{2N+2α+4}{N})$,
$\{\frac{2N+2α+4}{N}\}$, and $(\frac{2N+2α+4}{N},\frac{2N+2α}{N-2})$. Employing variational methods, we demonstrate the existence of a normalized ground state for the system in the mass subcritical, critical, and supercritical cases. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2511_15103 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Normalized solutions to subcritical Choquard systems with double couplings Pei, Wenliang Deng, Chonghao Analysis of PDEs 35J15, 35J60, 35Q55 We consider the Choquard system with both linear and nonlinear couplings $-Δu + μ_1 u =λ_1 ( I_α* |u|^{r_1} ) |u|^{r_1-2} u + βp( I_α* |v|^q)|u|^{p-2} u + κv,$ $-Δv + μ_2 v =λ_2 ( I_α* |v|^{r_2} ) |v|^{r_2-2} v + βq( I_α* |u|^p)|v|^{q-2} v + κu , $ $\int_{\mathbb{R}^N} u^2 = ρ_1^2\, , \int_{\mathbb{R}^N} v^2 = ρ_2^2,$ where $N \in \{3,4\}$, $λ_1, λ_2, β, κ, ρ_1,ρ_2 > 0$, $2_{α,*} :=\frac{N+α}{N} <p,q , r_1, r_2 <2_α^*:=\frac{N+α}{N-2}$ and $p+q\leq 2r_1 \leq 2r_2$ . We investigate a classification result as the parameters $p+q$, $2r_1$ and $2r_2$ vary across the ranges $(\frac{2N+2α}{N},\frac{2N+2α+4}{N})$, $\{\frac{2N+2α+4}{N}\}$, and $(\frac{2N+2α+4}{N},\frac{2N+2α}{N-2})$. Employing variational methods, we demonstrate the existence of a normalized ground state for the system in the mass subcritical, critical, and supercritical cases. |
| title | Normalized solutions to subcritical Choquard systems with double couplings |
| topic | Analysis of PDEs 35J15, 35J60, 35Q55 |
| url | https://arxiv.org/abs/2511.15103 |