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Chaos Solitons & Fractals

Quantum corrections to the modulational instability of Bose–Einstein condensates with two- and three-body interactions

Olivier Tiokeng Lekeufack, Subramaniyan Sabari, Serge Bruno Yamgoué, Kuppuswamy Porsezian, Timoléon Crépin Kofané

Published Apr 10, 2015• 12 citations
Publisher
DOI
10.1016/j.chaos.2015.03.015

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In this paper, we consider the coupled Gross-Pitaevskii (CGP) equations in a quasi-one dimensional geometry, which are governed by the dynamics of the coupled Bose Einstein condensations (BECs) in the presence of the three body interaction potential. Using the linear stability analysis (LSA), we obtain the dispersion relation for the system of coupled BECs. Analytically, we obtain a new explicit expression for the growth rate. Besides, we investigate the modulational instability (MI) criterion of constant amplitude of both uncoupled and coupled BECs for different values of the three body interaction potential. Finally, we compare our results of both uncoupled and coupled BECs in the presence and absence of three body interaction term.

•Feb 8, 2006•0 citations
We investigate analytically and numerically the modulational instability of a Bose-Einstein condensate with both two- and three-body interatomic interactions and trapped in an external parabolic potential. Analytical investigations performed lead us to establish an explicit time-dependent criterion for the modulational instability of the condensate. The effects of the potential as well as of the quintic nonlinear interaction are studied. Direct numerical simulations of the Gross-Pitaevskii equation with two- and three-body interactions describing the dynamics of the condensate agree with the analytical predictions.
Motivated by the recent experiment [Nature 530 (2016) 194] in which a stable droplet in a dipolar quantum gas has been created by the interaction-induced instability, we focus on the modulation instability of an optically-trapped dipolar Bose–Einstein condensate with three-body interaction. Within the mean-field level, we analytically solve the discrete cubic-quintic Gross–Pitaevskii equation with dipole–dipole interaction loaded into a deep optical lattice and show how combined effects of the three-body interaction and dipole–dipole interaction on the condition of modulational instability. Our results show that the interplay of the three-body interaction and dipole–dipole interaction can dramatically change the modulation instability condition compared with the ordinary Gross–Pitaevskii equation. We believe that the predicted results in this work can be useful for the future possible experiment of loading a Bose–Einstein condensate of 164 Dy atoms with strong magnetic dipole–dipole interaction into an optical lattice.
In this paper, we consider the coupled Gross-Pitaevskii (CGP) equations in a quasi-one dimensional geometry, which are governed by the dynamics of the coupled Bose Einstein condensations (BECs) in the presence of the three body interaction potential. Using the linear stability analysis (LSA), we obtain the dispersion relation for the system of coupled BECs. Analytically, we obtain a new explicit expression for the growth rate. Besides, we investigate the modulational instability (MI) criterion of constant amplitude of both uncoupled and coupled BECs for different values of the three body interaction potential. Finally, we compare our results of both uncoupled and coupled BECs in the presence and absence of three body interaction term.