From Short-Range to Mean-Field Models in Quantum Lattices

TL;DR

This paper rigorously connects short-range quantum lattice models with mean-field models via the Kac limit, showing convergence of equilibrium states and enabling better understanding of phase transitions in large-range interactions.

Contribution

It establishes a precise mathematical relation between short-range and mean-field quantum models, including convergence of all correlation functions and accommodating complex interaction components.

Findings

Proves convergence of equilibrium states in the long-range limit.

Allows for a continuum of long-range interaction components.

Extends results to general short-range Hamiltonians.

Abstract

Realistic effective interparticle interactions of quantum many-body systems are widely seen as being short-range. However, the rigorous mathematical analysis of this type of model turns out to be extremely difficult, in general, with many important fundamental questions remaining open still nowadays. By contrast, mean-field models come from different approximations or Ans\"{a}tze, and are thus less realistic, in a sense, but are technically advantageous, by allowing explicit computations while capturing surprisingly well many real physical phenomena. Here, we establish a precise mathematical relation between mean-field and short-range models, by using the long-range limit that is known in the literature as the Kac limit. If both attractive and repulsive long-range forces are present then it turns out that the limit mean-field model is not necessarily what one traditionally guesses. One important innovation of our study, in contrast with previous works on the subject, is the fact that we are able to show the convergence of equilibrium states, i.e., of all correlation functions. This paves the way for studying phase transitions, or at least important fingerprints of them like strong correlations at long distances, for models having interactions whose ranges are finite, but very large. It also sheds a new light on mean-field models. Even on the level of pressures, our results go considerably further than previous ones, by allowing, for instance, a continuum of long-range interaction components, as well as very general short-range Hamiltonians for the "free" part of the model.