Microscopic scattering theory for interacting bosons in weak random potentials
arXiv:1307.4940 · doi:10.1088/1367-2630/15/11/115015
Abstract
We develop a diagrammatic scattering theory for interacting bosons in a three-dimensional, weakly disordered potential. Based on a microscopic N-body scattering theory, we identify the relevant diagrams including elastic and inelastic collision processes that are sufficient to describe diffusive quantum transport. By taking advantage of the statistical properties of the weak disorder potential, we demonstrate how the N-body dynamics can be reduced to a nonlinear integral equation of Boltzmann type for the single-particle diffusive flux. Our theory reduces to the Gross-Pitaevskii mean field description in the limit where only elastic collisions are taken into account. However, even at weak interaction strength, inelastic collisions lead to energy redistribution between the bosons - initially prepared all at the same single-particle energy - and thereby induce thermalization of the single-particle current. In addition, we include also weak localization effects and determine the coherent corrections to the incoherent transport in terms of the coherent backscattering signal. We find that inelastic collisions lead to an enhancement of the backscattered cone in a narrow spectral window for increasing interaction strength.
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Cited by in corpus (10)
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- Localization of wave packets in one-dimensional random potentials
- Charge and spin diffusion on the metallic side of the metal-insulator transition: a self-consistent approach
- Localization landscape for interacting Bose gases in one-dimensional speckle potentials
- Al'tshuler-Aronov-Spivak oscillations of bosonic matter-wave beams in the presence of interaction
- Inversion of coherent backscattering with interacting Bose-Einstein condensates in two-dimensional disorder : a Truncated Wigner approach