Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid

In a joint experimental and theoretical effort, we report on the formation of a macrodroplet state in an ultracold bosonic gas of erbium atoms with strong dipolar interactions. By precise tuning of the s-wave scattering length below the so-called dipolar length, we observe a smooth crossover of the...

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Main Authors: L. Chomaz, S. Baier, D. Petter, M. J. Mark, F. Wächtler, L. Santos, F. Ferlaino
Format: Article
Language:English
Published: American Physical Society 2016-11-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.6.041039
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spelling doaj-b88722703b6f47ef86ce9a4e9ea7287a2020-11-24T23:38:18ZengAmerican Physical SocietyPhysical Review X2160-33082016-11-016404103910.1103/PhysRevX.6.041039Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum FluidL. ChomazS. BaierD. PetterM. J. MarkF. WächtlerL. SantosF. FerlainoIn a joint experimental and theoretical effort, we report on the formation of a macrodroplet state in an ultracold bosonic gas of erbium atoms with strong dipolar interactions. By precise tuning of the s-wave scattering length below the so-called dipolar length, we observe a smooth crossover of the ground state from a dilute Bose-Einstein condensate to a dense macrodroplet state of more than 2×10^{4}  atoms. Based on the study of collective excitations and loss features, we prove that quantum fluctuations stabilize the ultracold gas far beyond the instability threshold imposed by mean-field interactions. Finally, we perform expansion measurements, showing that although self-bound solutions are prevented by losses, the interplay between quantum stabilization and losses results in a minimal time-of-flight expansion velocity at a finite scattering length.http://doi.org/10.1103/PhysRevX.6.041039
collection DOAJ
language English
format Article
sources DOAJ
author L. Chomaz
S. Baier
D. Petter
M. J. Mark
F. Wächtler
L. Santos
F. Ferlaino
spellingShingle L. Chomaz
S. Baier
D. Petter
M. J. Mark
F. Wächtler
L. Santos
F. Ferlaino
Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
Physical Review X
author_facet L. Chomaz
S. Baier
D. Petter
M. J. Mark
F. Wächtler
L. Santos
F. Ferlaino
author_sort L. Chomaz
title Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
title_short Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
title_full Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
title_fullStr Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
title_full_unstemmed Quantum-Fluctuation-Driven Crossover from a Dilute Bose-Einstein Condensate to a Macrodroplet in a Dipolar Quantum Fluid
title_sort quantum-fluctuation-driven crossover from a dilute bose-einstein condensate to a macrodroplet in a dipolar quantum fluid
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2016-11-01
description In a joint experimental and theoretical effort, we report on the formation of a macrodroplet state in an ultracold bosonic gas of erbium atoms with strong dipolar interactions. By precise tuning of the s-wave scattering length below the so-called dipolar length, we observe a smooth crossover of the ground state from a dilute Bose-Einstein condensate to a dense macrodroplet state of more than 2×10^{4}  atoms. Based on the study of collective excitations and loss features, we prove that quantum fluctuations stabilize the ultracold gas far beyond the instability threshold imposed by mean-field interactions. Finally, we perform expansion measurements, showing that although self-bound solutions are prevented by losses, the interplay between quantum stabilization and losses results in a minimal time-of-flight expansion velocity at a finite scattering length.
url http://doi.org/10.1103/PhysRevX.6.041039
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