Derivation of the 1d NLS equation from the 3d quantum many-body dynamics of strongly confined bosons
arXiv:1803.11011 · doi:10.1063/1.5075514
Abstract
We consider the dynamics of interacting bosons initially exhibiting Bose-Einstein condensation. Due to an external trapping potential, the bosons are strongly confined in two spatial directions, with the transverse extension of the trap being of order . The non-negative interaction potential is scaled such that its scattering length is positive and of order , the range of the interaction scales as for . We prove that in the simultaneous limit and , the condensation is preserved by the dynamics and the time evolution is asymptotically described by a cubic defocusing nonlinear Schrödinger equation in one dimension, where the strength of the nonlinearity depends on the interaction and on the confining potential. This is the first derivation of a lower-dimensional effective evolution equation for singular potentials scaling with and lays the foundations for the derivation of the physically relevant one-dimensional Gross-Pitaevskii equation (). For our analysis, we adapt an approach by Pickl to the problem with strong confinement.
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Cited by in corpus (5)
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- Higher order corrections to the mean-field description of the dynamics of interacting bosons
- Derivation of the 1d Gross-Pitaevskii equation from the 3d quantum many-body dynamics of strongly confined bosons
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- On the nonlinear Schrödinger equation with a toroidal trap in the strong confinement regime