A two-atom dimer on a spherical surface has an angular-momentum-dependent binding energy and wave function, becoming squeezed and quasi-one-dimensional at high total angular momentum.
Probing the hollowing transition of a shell-shaped BEC with collective excitation
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abstract
We investigate the hollowing transition of a shell-shaped Bose-Einstein condensate using collective excitations. The shell is created using an immiscible dual-species BEC mixture, with its hollowness controlled by tuning the repulsive interspecies interaction via a Feshbach resonance. Our results reveal two distinct monopole modes in which the two condensates oscillate either in-phase or out-of-phase. The spectrum of the out-of-phase mode exhibits a non-monotonic dependence on the interspecies interaction, providing a clear signature of the topology change from a filled to a hollow condensate. Furthermore, we find that the critical point of the hollowing transition depends strongly on the number ratio of the two species. Our findings provide a detailed understanding of the topology change in shell-shaped quantum gases and pave the way for future study of quantum many-body phenomena in curved spaces.
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Dimer problem on a spherical surface
A two-atom dimer on a spherical surface has an angular-momentum-dependent binding energy and wave function, becoming squeezed and quasi-one-dimensional at high total angular momentum.