2017
DOI: 10.1103/physreva.95.023622
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Phases of dipolar bosons in a bilayer geometry

Abstract: We study by first principle computer simulations the low temperature phase diagram of bosonic dipolar gases in a bilayer geometry, as a function of the two control parameters, i.e., the in-plane density and the interlayer distance. We observe four distinct phases, namely paired and decoupled superfluids, as well as a crystal of dimers and one consisting of two aligned crystalline layers. A direct quantum phase transition from a dimer crystal to two independent superfluids is observed in a relatively wide range… Show more

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Cited by 24 publications
(28 citation statements)
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“…As the density is increased, the potential energy starts to dominate and a triangular crystal is formed. For large separation between layers, two independent atomic crystals are formed and the phase transition occurs when the density per layer reaches the same critical value as in a single-layer geometry, n A r 2 0 = n B r 2 0 ≈ 290 [142,145]. In the limit of small interlayer separations, a single molecular crystal is formed at the density nr 2 0 ≈ 9.…”
Section: Phase Diagrammentioning
confidence: 99%
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“…As the density is increased, the potential energy starts to dominate and a triangular crystal is formed. For large separation between layers, two independent atomic crystals are formed and the phase transition occurs when the density per layer reaches the same critical value as in a single-layer geometry, n A r 2 0 = n B r 2 0 ≈ 290 [142,145]. In the limit of small interlayer separations, a single molecular crystal is formed at the density nr 2 0 ≈ 9.…”
Section: Phase Diagrammentioning
confidence: 99%
“…(7.1) we anticipate to find three phases: atomic gas, solid, and gas of chains. This comes from considering previous studies in a dipolar layer [30,31] and bilayer [32,33,145].…”
Section: The Hamiltonianmentioning
confidence: 99%
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“…As the density of the liquid is increased, the potential energy starts to dominate and eventually a triangular crystal is formed. For large separation between layers, two independent atomic crystals are formed and the phase transition occurs when the density per layer reaches the same critical value as in a single-layer geometry, nr 2 0 ≈ 290 [17,22]. In the limit of small interlayer separations, a single molecular crystal is formed at density nr 2 0 ≈ 9.…”
mentioning
confidence: 99%
“…Quantum gases with dipolar interaction are also explored with cold atoms. In these systems, dipolar interactions lead to droplet structures with spatial ordering and coherence [36][37][38][39][40], few-body complexes [41,42], and pair superfluid and crystal phases in bilayers of dipoles [43][44][45][46].…”
mentioning
confidence: 99%