paper

Existence of ground state solutions to Kirchhoff--Choquard system in with constant potentials

arXiv:2507.09163

Abstract

In this paper, we consider the following linearly coupled Kirchhoff--Choquard system in : \begin{align*} \begin{cases} -\left(a_1 + b_1\int_{\mathbb{R}^3} |\nabla u|^2\,dx\right)Δu + V_1 u = μ(I_α * |u|^p) |u|^{p - 2} u + λv, \ \ x\in\mathbb{R}^3\\ -\left(a_2 + b_2\int_{\mathbb{R}^3} |\nabla v|^2\,dx\right)Δv + V_2 v = ν(I_α * |v|^q) |v|^{q - 2} v + λu,\ \ x\in\mathbb{R}^3 \\ u, v \in H^1(\mathbb{R}^3), \end{cases} \end{align*} where , , and are positive constants. The function denotes the Riesz potential with . We study the existence of positive ground state solutions under the conditions , or , or . Assuming suitable conditions on , , and , we obtain a ground state solution by employing a variational approach based on the Nehari--Pohozaev manifold, inspired by the works of Ueno (Commun. Pure Appl. Anal. 24 (2025)) and Chen--Liu (J. Math. Anal. 473 (2019)). In particular, we emphasize that in the upper half critical case and the lower half critical case , a ground state solution can still be obtained by taking or sufficiently large to control the energy level of the minimization problem. To employ the Nehari--Pohozaev manifold we extend a regularity result to the linearly coupled system, which is essential for the validity of the Pohozaev identity.

35 pages