2018
DOI: 10.1088/1361-6455/aaa116
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Few-body physics in resonantly interacting ultracold quantum gases

Abstract: We provide a general discussion on the importance of three-body Efimov physics for strongly interacting ultracold quantum gases. Using the adiabatic hyperspherical representation, we discuss a universal classification of three-body systems in terms of the attractive or repulsive character of the effective interactions. The hyperspherical representation leads to a simple and conceptually clear picture for the bound and scattering properties of three-body systems with strong s-wave interactions. Using our univer… Show more

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Cited by 96 publications
(153 citation statements)
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References 278 publications
(1,177 reference statements)
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“…Therefore, we conclude that the potentials V (1) sc and V (2) sc are too shallow to obey the van der Waals universality in Re(D). Furthermore, we find a sharp minimum in −Im(D) for V (1) sc at a/r vdW = 0.739 which is likely to be caused by destructive interference between competing pathways for three-body recombination [17]. Figure S3: Three-body scattering hypervolume D corresponding to soft-core van der Waals potentials supporting one, two and three s-wave dimer states as a function of the two-body scattering length a.…”
Section: Additional Results For the Soft-core Van Der Waals Potementioning
confidence: 98%
“…Therefore, we conclude that the potentials V (1) sc and V (2) sc are too shallow to obey the van der Waals universality in Re(D). Furthermore, we find a sharp minimum in −Im(D) for V (1) sc at a/r vdW = 0.739 which is likely to be caused by destructive interference between competing pathways for three-body recombination [17]. Figure S3: Three-body scattering hypervolume D corresponding to soft-core van der Waals potentials supporting one, two and three s-wave dimer states as a function of the two-body scattering length a.…”
Section: Additional Results For the Soft-core Van Der Waals Potementioning
confidence: 98%
“…For strongly interacting Bose gases, there is an additional complication due to the existence of the threebody Efimov effect. At unitarity (a → ∞) an infinity of three-body trimers emerges, which strongly alters the scattering observables at ultracold energies [6][7][8][9]. Here, universal relations between few-body physics and macroscopic observables also involve the three-body contact density C 3 [10,11], central to the many-body theory, whose properties are not yet theoretically known for the degenerate Bose gas in the unitary regime.…”
Section: Dynamics Of Three-body Correlations In Quenched Unitary Bosementioning
confidence: 99%
“…These developments have stimulated much recent theoretical and experimental progress, as reviewed in Refs. [11][12][13].…”
Section: Introductionmentioning
confidence: 99%