{ "id": "math-ph/0606017", "version": "v3", "published": "2006-06-05T22:41:59.000Z", "updated": "2006-12-10T09:44:01.000Z", "title": "Derivation of the Gross-Pitaevskii Equation for the Dynamics of Bose-Einstein Condensate", "authors": [ "Laszlo Erdos", "Benjamin Schlein", "Horng-Tzer Yau" ], "comment": "Latex file, 66 pages; new version, with an appendix to include a new class of inital states", "categories": [ "math-ph", "math.MP" ], "abstract": "Consider a system of $N$ bosons in three dimensions interacting via a repulsive short range pair potential $N^2V(N(x_i-x_j))$, where $\\bx=(x_1, >..., x_N)$ denotes the positions of the particles. Let $H_N$ denote the Hamiltonian of the system and let $\\psi_{N,t}$ be the solution to the Schr\\\"odinger equation. Suppose that the initial data $\\psi_{N,0}$ satisfies the energy condition \\[ < \\psi_{N,0}, H_N^k \\psi_{N,0} > \\leq C^k N^k \\] for $k=1,2,... $. We also assume that the $k$-particle density matrices of the initial state are asymptotically factorized as $N\\to\\infty$. We prove that the $k$-particle density matrices of $\\psi_{N,t}$ are also asymptotically factorized and the one particle orbital wave function solves the Gross-Pitaevskii equation, a cubic non-linear Schr\\\"odinger equation with the coupling constant given by the scattering length of the potential $V$. We also prove the same conclusion if the energy condition holds only for $k=1$ but the factorization of $\\psi_{N,0}$ is assumed in a stronger sense.", "revisions": [ { "version": "v3", "updated": "2006-12-10T09:44:01.000Z" } ], "analyses": { "subjects": [ "35Q55", "81Q15", "81T18", "81V70" ], "keywords": [ "gross-pitaevskii equation", "bose-einstein condensate", "particle density matrices", "energy condition", "derivation" ], "note": { "typesetting": "LaTeX", "pages": 66, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2006math.ph...6017E" } } }