On the $L^2$ Rate of Convergence in the Limit from the Hartree to the Vlasov$\unicode{x2013}$Poisson Equation
Jacky J. Chong, Laurent Lafleche, Chiara Saffirio
TL;DR
The paper rigorously characterizes the semiclassical limit $\hbar\to 0$ of the Hartree equation with Coulomb interactions, showing that the Wigner transform of the Hartree solution converges in $L^2$ to a Vlasov–Poisson solution at a rate linear in $\hbar$. A novel stability framework for the square root of phase-space densities is developed, together with Wick quantization to overcome positivity issues and obtain explicit, uniform-in-$\hbar$ bounds. The analysis introduces quantum Sobolev-type spaces and detailed commutator estimates, enabling a precise, quantitative comparison between quantum and classical evolutions in the Schatten norm setting. The results improve previous rates and offer a method that parallels mean-field derivations for mixed quantum states, with potential insights for the quantum-to-classical transition in many-body dynamics. The work thus provides a sharp, practically applicable link between quantum Hartree dynamics and classical Vlasov–Poisson dynamics in the singular Coulomb regime.
Abstract
Using a new stability estimate for the difference of the square roots of two solutions of the Vlasov$\unicode{x2013}$Poisson equation, we obtain the convergence in the $L^2$ norm of the Wigner transform of a solution of the Hartree equation with Coulomb potential to a solution of the Vlasov$\unicode{x2013}$Poisson equation, with a rate of convergence proportional to $\hbar$. This improves the $\hbar^{3/4-\varepsilon}$ rate of convergence in $L^2$ obtained in [L.~Lafleche, C.~Saffirio: Analysis & PDE, to appear]. Another reason of interest of this paper is the new method, reminiscent of the ones used to prove the mean-field limit from the many-body Schrödinger equation towards the Hartree$\unicode{x2013}$Fock equation for mixed states.
