Two-Step Production of Resonant Bose-Einstein Condensates

Abstract

Producing a substantial and stable resonant Bose-Einstein condensate (BEC) has proven to be a challenging experimental task due to heating and three-body losses that may occur even before the gas comes to thermal equilibrium. In this paper, by considering only two-body correlations, we note that a sudden quench from small to large scattering lengths may not be the best way to prepare a resonant BEC. As an alternative, we propose a two-step scheme that involves an intermediate scattering length, between $0$ and $\infty$, which serves to maximize the transfer probability of $N$ bosons of mass $m$ in a harmonic trap with frequency $\omega$. We find that the intermediate scattering length should be $a\approx 3.16N^{-2/3}\sqrt{\hslash /(m\omega )}$ to produce an optimum transition probability of $1.03N^{-1/6}$.

References in corpus (5)

• Two and Three-body Contacts in the Unitary Bose Gas
• Universal Scaling Laws in the Dynamics of a Homogeneous Unitary Bose Gas
• Ground State Properties of Cold Bosonic Atoms At Large Scattering Lengths
• Monte Carlo Simulations of the Unitary Bose Gas
• Bose Gases Near Resonance: renormalized interactions in a condensate

Cited by in corpus (1)

• Bunching, clustering, and the buildup of few-body correlations in a quenched unitary Bose gas