Large deviations for trapped interacting brownian particles and paths
成果类型:
Article
署名作者:
Adams, Stefan; Bru, Jean-Bernard; Koenig, Wolfgang
署名单位:
Max Planck Society; Dublin Institute for Advanced Studies; Johannes Gutenberg University of Mainz; Leipzig University
刊物名称:
ANNALS OF PROBABILITY
ISSN/ISSBN:
0091-1798
DOI:
10.1214/009117906000000214
发表日期:
2006
页码:
1370-1422
关键词:
bose-einstein condensation
gas
systems
polaron
vortex
energy
摘要:
We introduce two probabilistic models for N interacting Brownian motions moving in a trap in R-d under mutually repellent forces. The two models are defined in terms of transformed path measures on finite time intervals under a trap Hamiltonian and two respective pair-interaction Hamiltonians. The first pair interaction exhibits a particle repellency, while the second one imposes a path repellency. We analyze both models in the limit of diverging time with fixed number N of Brownian motions. In particular, we prove large deviations principles for the normalized occupation measures. The minimizers of the rate functions are related to a certain associated operator, the Hamilton operator for a system of N interacting trapped particles. More precisely, in the particle-repellency model, the minimizer is its ground state, and in the path-repellency model, the minimizers are its ground product-states. In the case of path-repellency, we also discuss the case of a Dirac-type interaction, which is rigorously defined in terms of Brownian intersection local times. We prove a large-deviation result for a discrete variant of the model. This study is a contribution to the search for a mathematical formulation of the quantum system of N trapped interacting bosons as a model for Bose-Einstein condensation, motivated by the success of the famous 1995 experiments. Recently, Lieb et al. described the large-N behavior of the ground state in terms of the well-known Gross-Pitaevskii formula, involving the scattering length of the pair potential. We prove that the large-N behavior of the ground product-states is also described by the Gross-Pitaevskii formula, however, with the scattering length of the pair potential replaced by its integral.