Thermodynamic limit and $L^{\infty }$-convergence rate for the cubic-quintic Schrödinger model

Abstract

We investigate the thermodynamic limit for the cubic-quintic Schrödinger model as the size of the domain tends to infinity with fixed density $\rho =N/|\mathcal{D}|$, where $N$ denotes particle number and $|\mathcal{D}|$ denotes the volume of the bounded domain $\mathcal{D}\subset {\mathbb{R}}^d$ ($d=1,2,3$). We firstly prove the existence of thermodynamic limit, which is equal to $-\frac{3}{32}$ for \(0<ρ\leq \frac{3}{4}\), while $-\left(\frac{1}{2}-\frac{\rho }{3}\right)\frac{\rho }{2}$ for $\frac{3}{4}<\rho \le 1$. When \(0<ρ<1\) and \(\mathcal{D}\) is a spherical domain, we further show that, up to a scaling, the ground state of the cubic-quintic Schrödinger energy will converge strongly to a Thomas-Fermi ground state in $L^2\cap L^6$. Finally, we obtain the $L^{\infty }$-convergence rate of ground states for \(0<ρ<3/4\) by developing a novel method, including some iterative techniques, uniform energy estimates and gradient estimates. We believe this method is applicable to other general nonlinearities.

34 pages. arXiv admin note: text overlap with arXiv:2410.14300