2012
DOI: 10.1088/1751-8113/45/20/205302
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Universal two-body spectra of ultracold harmonically trapped atoms in two and three dimensions

Abstract: Abstract. We consider the spectrum of two ultracold harmonically trapped atoms interacting via short-range interactions. The Green's function approach is used to unify the two and three dimensional cases. We derive criteria for the universality of the spectrum, i.e. its independence of the details of the short-range interaction. The results in three dimensions are examplified for narrow s-wave Feshbach resonances and we show how effective range corrections can modify the rearrangement of the level structure. H… Show more

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Cited by 24 publications
(19 citation statements)
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“…This is very similar to what is seen in other confined systems such as short-range interacting two-body systems in a harmonic trap [56]. The latter show similar jumps as function of the ratio of the interaction and confinement energy scales and have been related to the Zeldovich rearrangement effect seen for particles in strong magnetic fields [57,58].…”
Section: Trimer Energy With Periodic Boundary Conditionssupporting
confidence: 84%
“…This is very similar to what is seen in other confined systems such as short-range interacting two-body systems in a harmonic trap [56]. The latter show similar jumps as function of the ratio of the interaction and confinement energy scales and have been related to the Zeldovich rearrangement effect seen for particles in strong magnetic fields [57,58].…”
Section: Trimer Energy With Periodic Boundary Conditionssupporting
confidence: 84%
“…Another interesting direction in which the harmonic model can be used is for the study of higher-order terms in the interaction such as those coming from effectiverange corrections to the model of Busch et al [18,43]. Recent experiments have shown a potential need for such corrections in both two- [44] and three-dimensional cold atomic gas systems [45].…”
Section: Discussionmentioning
confidence: 99%
“…The lack of symmetry between primed and unprimed coordinates in (25) is deceiving. One can either use the definition (22) or the properties of 3 F 2 (· · · ; · ·; ·) to show that R(ν , µ , ν, µ) = R(ν, µ, ν , µ ).…”
Section: Symmetries and The Superselection Rulementioning
confidence: 99%