Rate of convergence towards equations of Hartree type for mixture condensates with factorized initial data
arXiv:1907.03388 · doi:10.1063/5.0019679
Abstract
We consider a system of components of bosons, each of which consists of particles, respectively. The bosons are in three dimensions with interactions via a generalized interaction potential which includes the Coulomb interaction. We set the initial condition to describe a mixture condensate, i.e., a tensor product of factorized states. We show that the difference between the many-body Schrödinger evolution in the mean-field regime and the corresponding -particle dynamics due to a system of Hartree equation is where .
arXiv admin note: text overlap with arXiv:1811.04984 by other authors
References in corpus (11)
- Creation of ultracold RbCs molecules in the rovibrational ground state
- Observation of Heteronuclear Feshbach Molecules from a Rb - Rb gas
- Optimal Rate for Bose-Einstein Condensation in the Gross-Pitaevskii Regime
- Gross-Pitaevskii Dynamics for Bose-Einstein Condensates
- Complete Bose-Einstein condensation in the Gross-Pitaevskii regime
- Rate of Convergence in Nonlinear Hartree Dynamics with Factorized Initial Data
- Derivation of the Hartree equation for compound Bose gases in the mean field limit
- Rate of Convergence towards Hartree Dynamics with Singular Interaction Potential
- Mean-field dynamics for mixture condensates via Fock space methods
- Convergence rate towards the fractional Hartree-equation with singular potentials in higher Sobolev norms
- On the time dependence of the rate of convergence towards Hartree dynamics for interacting Bosons
Cited by in corpus (4)
- On the characterisation of fragmented Bose-Einstein condensation and its emergent effective evolution
- Properties of a trapped multiple-species bosonic mixture at the infinite-particle-number limit: A solvable model
- Fragmentation of a trapped multiple-species bosonic mixture
- Uniform in Time Convergence to Bose-Einstein Condensation for a Weakly Interacting Bose Gas with an External Potential