Spinor Boson Droplets Stabilized By Spin Fluctuations
arXiv:2201.09628 · doi:10.1103/PhysRevA.105.043309
Abstract
Self-trapped droplets stabilized by quantum fluctuations have been experimentally realized in dipolar gases and binary Boson mixtures. We propose spinor Bose gases as another candidate for droplet formation in this work. For spin-1 gas, we find that spin fluctuations give a dilute but self-trapped state for two different order parameters where the mean-field picture predicts collapse. A polar droplet phase can be stabilized by spin fluctuations for both antiferromagnetic and ferromagnetic spin-dependent coupling. An antiferromagnetic droplet phase can be stabilized similarly with a negative quadratic Zeeman shift. Furthermore, the beyond mean-field energy of the system depends on the quadratic Zeeman coupling, which provides a mechanism to tune the droplet formation and its density. We discuss the parameters necessary for the experimental realization of such spinor droplets.
8 pages, 4 figures
References in corpus (10)
- Quantum liquid droplets in a mixture of Bose-Einstein condensates
- Self-bound droplets of a dilute magnetic quantum liquid
- Formation of bright matter-wave solitons during the collapse of Bose-Einstein condensates
- Bragg spectroscopy of a strongly interacting 85Rb Bose-Einstein condensate
- Spinor Dynamics in an Antiferromagnetic Spin-1 Condensate
- Observation of deviations from ideal gas thermodynamics in a trapped Bose-Einstein condensed gas
- Effects of Interactions on the Critical Temperature of a Trapped Bose Gas
- Beyond Lee-Huang-Yang description of self-bound Bose mixtures
- Dynamics of F=1 87Rb condensates at finite temperatures
- Observation of a strongly ferromagnetic spinor Bose-Einstein condensate