Derivation of the Bose-Hubbard model in the multiscale limit
Reika Fukuizumi, Andrea Sacchetti

TL;DR
This paper rigorously derives the Bose-Hubbard model from a one-dimensional nonlinear Schrödinger equation with a periodic potential, demonstrating phase transition behavior in Bose-Einstein condensates.
Contribution
It provides a mathematical proof connecting the nonlinear Schrödinger equation to the Bose-Hubbard model in the multiscale limit, including phase transition analysis.
Findings
Stationary solutions of the Bose-Hubbard model approximate those of the NLSE in the semiclassical limit.
Large nonlinearity leads to localized solutions on a single lattice site.
Phase transition from superfluid to Mott-insulator is rigorously established.
Abstract
In this paper we consider a one-dimensional non-linear Schroedinger equation (NLSE) with a periodic potential. In the semiclassical limit we prove that the stationary solutions of the Bose-Hubbard equation approximate the stationary solutions of the (NLSE). In particular, in the limit of large nonlinearity strength the stationary solutions turn out to be localized on a single lattice site of the periodic potential; as a result the phase transition from superfluid to Mott-insulator phase for Bose-Einstein condensates in a one-dimensional periodic lattice is rigorously proved.
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Taxonomy
TopicsCold Atom Physics and Bose-Einstein Condensates · Quantum, superfluid, helium dynamics · Quantum many-body systems
