Crossing the superfluid-supersolid transition of an elongated dipolar condensate
arXiv:2207.07711 · doi:10.1103/PhysRevA.106.043313
Abstract
We provide a theoretical characterization of the dynamical crossing of the superfluid-supersolid phase transition for a dipolar condensate confined in an elongated trap, as observed in the recent experiment by G. Biagioni et al. [Phys. Rev. X 12, 021019 (2022)]. By means of the extended Gross-Pitaevskii theory, which includes the Lee-Huang-Yang quantum fluctuation correction, we first analyze the ground state configurations of the system as a function of the interparticle scattering length, for both trap configurations employed in the experiment. Then, we discuss the effects of the ramp velocity, by which the scattering length is tuned across the transition, on the collective excitations of the system in both the superfluid and supersolid phases. We find that, when the transverse confinement is sufficiently strong and the transition has a smooth (continuous) character, the system essentially displays a (quasi) 1D behavior, its excitation dynamics being dominated by the axial breathing modes. Instead, for shallower transverse trapping, when the transition becomes discontinuous, the collective excitations of the supersolid display a coupling with the transverse modes, signalling the onset of a dimensional crossover.
9 pages, 8 figures
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Cited by in corpus (6)
- Supersolidity and crystallization of a dipolar Bose gas in an infinite tube
- Supersolid formation in a dipolar condensate by roton instability
- Kibble-Zurek scaling of the superfluid-supersolid transition in an elongated dipolar gas
- Phase-induced vortex pinning in rotating supersolid dipolar systems
- Localized States in Dipolar Bose-Einstein Condensates: To be or not to be of second order
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