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Normalized Solutions for Schrödinger-Bopp-Podolsky Systems with Critical Choquard-Type Nonlinearity on Bounded Domains

Li Chen, Li Wang

TL;DR

The paper studies normalized solutions to a Schrödinger-Bopp-Podolsky system on a bounded domain with a critical Choquard-type nonlinearity. It reduces the problem by solving for the electrostatic potential $\phi$ as $\Phi(u)$, yielding a single-variable energy $J$ on the mass-constrained sphere $S_{r,b}$, and employs a truncation technique to obtain a coercive, bounded-below functional $J^T$ with a $(PS)_d$ condition. A genus-based minimax scheme applied to $J^T$ generates negative critical levels $d_k$, which correspond to critical points of the truncated functional; these are shown to be critical for the original functional, establishing the existence of at least $k$ normalized solutions for sufficiently small mass $b$. The results highlight multiplicity phenomena for nonlocal, gauge-field coupled systems on bounded domains under Navier-type constraints and nonuniform charge distributions $q(x)$, driven by a critical Choquard nonlinearity.

Abstract

In this paper, we study normalized solutions for the following critical Schrödinger-Bopp-Podolsky system: $$-Δu + q(x)φu = λu + |u|^{p-2}u + \bigl(I_α* |u|^{3+α}\bigr)|u|^{1+α}u,\quad \text{in } Ω_r,$$ $$-Δφ+ Δ^2φ= q(x)u^2, \ \qquad\qquad\qquad\qquad\qquad\qquad\qquad\ \text{ in } Ω_r,$$ where $Ω_r \subset \mathbb R^3$ is a smooth bounded domain, $p \in \left(2, \frac{8}{3}\right)$, $q(x) \in C(\barΩ_r) \backslash \{0\}$ and $λ\in \mathbb R$ is the Lagrange multiplier associated with the constraint $\int_{Ω_r} |u|^2\, \mathrm d x = b^2$ for some $b > 0$. Here $α> 0$, $I_α$ denotes the Riesz potential, and the domain parameter $r$ reflects the size of $Ω_r$ whose precise definition will be given in Section 3. By applying a special minimax principle together with a truncation technique, we prove that there exists $b^* > 0$ such that the system admits multiple normalized solutions whenever $b \in (0, b^*)$ under Navier boundary conditions.

Normalized Solutions for Schrödinger-Bopp-Podolsky Systems with Critical Choquard-Type Nonlinearity on Bounded Domains

TL;DR

The paper studies normalized solutions to a Schrödinger-Bopp-Podolsky system on a bounded domain with a critical Choquard-type nonlinearity. It reduces the problem by solving for the electrostatic potential as , yielding a single-variable energy on the mass-constrained sphere , and employs a truncation technique to obtain a coercive, bounded-below functional with a condition. A genus-based minimax scheme applied to generates negative critical levels , which correspond to critical points of the truncated functional; these are shown to be critical for the original functional, establishing the existence of at least normalized solutions for sufficiently small mass . The results highlight multiplicity phenomena for nonlocal, gauge-field coupled systems on bounded domains under Navier-type constraints and nonuniform charge distributions , driven by a critical Choquard nonlinearity.

Abstract

In this paper, we study normalized solutions for the following critical Schrödinger-Bopp-Podolsky system: where is a smooth bounded domain, , and is the Lagrange multiplier associated with the constraint for some . Here , denotes the Riesz potential, and the domain parameter reflects the size of whose precise definition will be given in Section 3. By applying a special minimax principle together with a truncation technique, we prove that there exists such that the system admits multiple normalized solutions whenever under Navier boundary conditions.
Paper Structure (7 sections, 10 theorems, 101 equations)

This paper contains 7 sections, 10 theorems, 101 equations.

Key Result

theorem 1

For any given $k \in \mathbb N$, there exist a constant $b^* > 0$, such that for every $b \in (0,b^*)$, the equation eq:1.1 subject to the boundary conditions eq:1.2-eq:1.3 admits at least k solutions satisfying the constraint for any $j = 1, 2, \cdots, k$.

Theorems & Definitions (12)

  • theorem 1: label=thm:1.1
  • lemma 1
  • lemma 2: label=lemma:2.2*, note=Gagliardo-Nirenberg inequality, 22
  • Proposition 2.1
  • lemma 3: label=lemma:2.3
  • lemma 4: label=lemma:2.4, note=24
  • lemma 5: label=lemma:2.5, note=24
  • lemma 6: label=lemma:3.1
  • proof
  • lemma 7: label=lemma:3.2
  • ...and 2 more