Abstract
We describe the ground state of a large, dilute, neutral atom Bose–Einstein condensate (BEC) doped with N strongly coupled mutually indistinguishable, bosonic neutral atoms (referred to as ‘impurity’) in the polaron regime where the BEC density response to the impurity atoms remains significantly smaller than the average density of the surrounding BEC. We find that N impurity atoms with N ≠ 1 can self-localize at a lower value of the impurity–boson interaction strength than a single impurity atom. When the ‘bare’ short-range impurity–impurity repulsion does not play a significant role, the self-localization of multiple bosonic impurity atoms into the same single particle orbital (which we call co-self-localization) is the nucleation process of the phase separation transition. When the short-range impurity–impurity repulsion successfully competes with co-self-localization, the system may form a stable liquid of self-localized single impurity polarons.
Highlights
Cold atom traps offer intriguing advantages for studying strong interaction physics in quantum many-body systems [1]
We describe the ground state of a large BEC with multiple, strongly coupled, mutually indistinguishable, bosonic impurity atoms embedded in a large dilute gas Bose-Einstein condensate
As we expect one and two-dimensional BEC or quasi-BEC systems to undergo phase separation as well as exhibit self-localization of impurity atoms, we suggest that a combination of a magnetically controlled Feshbach resonance and a confinement-induced resonance may access self-localized single impurity polaron fluids
Summary
Cold atom traps offer intriguing advantages for studying strong interaction physics in quantum many-body systems [1]. The cold atom realization of self-localized polarons with repulsive impurity-boson interactions can demonstrate polaron physics in regimes that are difficult to access in condensed matter [10]. Cold atom physics is poised to realize polarons of this type at strong coupling, creating structures that are smaller than the coherence length of the BEC. We describe the ground state of a large BEC with multiple, strongly coupled, mutually indistinguishable, bosonic impurity atoms embedded in a large dilute gas Bose-Einstein condensate.
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