Polarized Rabi-Coupled and Spinor Boson Droplets
arXiv:2210.08946 · doi:10.1103/PhysRevA.107.023322
Abstract
Self-bound quantum droplets form when the mean-field tendency of the gas to collapse is stabilized by the effectively repulsive beyond mean-field fluctuations. The beyond mean-field effects depend on Rabi-frequency and quadratic Zeeman effect for the Rabi-coupled Bose mixtures and the spinor gases, respectively. The effects of varying and on the quantum droplet have recently been examined for unpolarized Rabi-coupled Bose mixture with zero detuning and unpolarized spinor gas with . In this paper, we theoretically explore the stability of the droplet phase for polarized Rabi-coupled Bose mixture and spinor gas. We calculate the Lee-Huang-Yang corrections for both gases with polarized order parameters and obtain the phase diagram of the droplets on the parameter space of - and - for Rabi-coupled mixture and spinor gas, respectively. Finally, we highlight the similarities and differences between the two systems and discuss their experimental feasibility.
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Cited by in corpus (3)
- Breakdown of the single-mode description of ultradilute quantum droplets in binary Bose mixtures: A perspective from a microscopic bosonic pairing theory
- Nonuniversal equation of state for Rabi-coupled bosonic gases: a droplet phase
- Bose-Bose gases with nonuniversal corrections to the interactions: a droplet phase