Abstract

We present an exact analytical model of a cigar-shaped Bose-Einstein condensate at negative temperature. This work is motivated by the first experimental discovery of negative temperature in Bose-Einstein condensate by Braun et al. We have considered an external confinement which is a combination of expulsive trap, bi-chromatic optical lattice trap, and linear trap. The present method is capable of providing the exact form of the condensate wavefunction, phase, nonlinearity and gain/loss. One of the consistency conditions is shown to map onto the Schrödinger equation, leading to a significant control over the dynamics of the system. We have modified the model by replacing the optical lattice trap by a bi-chromatic optical lattice trap, which imparts better localization at the central frustrated site, delineated through the variation of condensate fraction. Estimation of temperature and a numerical stability analysis are also carried out. Incorporation of an additional linear trap introduces asymmetry and the corresponding temporal dynamics reveal atom distillation at negative temperature.

Highlights

  • This work is motivated by the first experimental discovery of negative temperature in Bose-Einstein condensate by Braun et al We have considered an external confinement which is a combination of expulsive trap, bi-chromatic optical lattice trap, and linear trap

  • We report a large class of exact solitary wave solutions for 1D-Bose-Einstein condensate (BEC) at negative temperature by exploiting a composite potential

  • Different combinations of external traps are explicated to broaden the scope for future applications

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Summary

Introduction

The localization of condensate density, which is the characteristic feature of a disordered potential, is observed corresponding to the variation of trap parameters in the negative temperature domain. We present the model for constructing exact solution of 1D-Gross Pitäevskii equation (GPE) at negative temperature under the composite confinement (a linear trap, an expulsive oscillator and a BOL trap) in presence of space- and time-modulated cubic nonlinearity and gain/loss. The axial compression of the atomic number density is observed with the variation of trap parameters, i.e., the power and wavelength of the lasers, and the expulsive oscillator frequency.

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