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Bulletin of the American Physical Society

Superfluid Hall effect in a Bose-Einstein condensate

Lindsay J. LeBlanc, Karina Jiménez-García, Ross Williams, Matthew C. Beeler, Abigail R. Perry, William D. Phillips, Ian B. Spielman

Published Jun 6, 2012• 0 citations
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This chapter discusses different phases of magnon superfluidity, including those in a magnetic trap; and signatures of magnon superfluidity: (i) spin supercurrent, which transports the magnetization for a macroscopic distance (up to 1 cm); (ii) spin current Josephson effect, which shows the interference between two condensates; (iii) spin current vortex — a topological defect which is an analog of a quantized vortex in superfluids, of an Abrikosov vortex in superconductors, and cosmic strings in relativistic theories; and (iv) Goldstone modes related to broken U(1) symmetry — phonons in the spin-superfluid magnon gas. The chapter also considers the topic of spin supercurrent in general, including spin-Hall and intrinsic quantum spin-Hall effects.
The anomalous Hall effect has had a profound influence on the understanding of many electronic topological materials but is much less studied in their bosonic counterparts. We predict that an intrinsic anomalous Hall effect exists in a recently realized bosonic chiral superfluid, a p-orbital Bose-Einstein condensate in a 2D hexagonal boron nitride optical lattice [Wang et al., Nature (London) 596, 227 (2021)NATUAS0028-083610.1038/s41586-021-03702-0]. We evaluate the frequency-dependent Hall conductivity within a multi-orbital Bose-Hubbard model that accurately captures the real experimental system. We find that in the high frequency limit, the Hall conductivity is determined by finite loop current correlations on the s-orbital residing sublattice, the latter a defining feature of the system's chirality. In the opposite limit, the dc Hall conductivity can trace its origin back to the noninteracting band Berry curvature at the condensation momentum, although the contribution from atomic interactions can be significant. We discuss available experimental probes to observe this intrinsic anomalous Hall effect at both zero and finite frequencies.