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

preprint2026arXivOpen access

Abstract

In this paper, we study normalized solutions for the following critical Schrödinger-Bopp-Podolsky system: −Δu+q(x)ϕu=λu+∣u∣p−2u+(Iα∗∣u∣3+α)∣u∣1+αu,in Ωr,-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+Δ2ϕ=q(x)u2,   in Ωr,-Δϕ+ Δ^2ϕ= q(x)u^2, \ \qquad\qquad\qquad\qquad\qquad\qquad\qquad\ \text{ in } Ω_r, where Ωr⊂R3Ω_r \subset \mathbb R^3 is a smooth bounded domain, p∈(2,83)p \in \left(2, \frac{8}{3}\right), q(x)∈C(Ωˉr)\{0}q(x) \in C(\barΩ_r) \backslash \{0\} and λ∈Rλ\in \mathbb R is the Lagrange multiplier associated with the constraint ∫Ωr∣u∣2 dx=b2\int_{Ω_r} |u|^2\, \mathrm d x = b^2 for some b>0b > 0. Here α>0α> 0, IαI_α denotes the Riesz potential, and the domain parameter rr reflects the size of ΩrΩ_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∗>0b^* > 0 such that the system admits multiple normalized solutions whenever b∈(0,b∗)b \in (0, b^*) under Navier boundary conditions.

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