2015
DOI: 10.1088/0953-4075/48/8/085301
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Three-body recombination of two-component cold atomic gases into deep dimers in an optical model

Abstract: We consider three-body recombination into deep dimers in a mass-imbalanced two-component atomic gas. We use an optical model where a phenomenological imaginary potential is added to the lowest adiabatic hyper-spherical potential. The consequent imaginary part of the energy eigenvalue corresponds to the decay rate or recombination probability of the three-body system. The method is formulated in details and the relevant qualitative features are discussed as functions of scattering lengths and masses. We use zer… Show more

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Cited by 29 publications
(22 citation statements)
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“…The existence of an infinite series of three-body bound states for resonant two-body interaction, as predicted by Efimov (Efimov, 1970), is not only present for homonuclear systems, as such universal three-body bound states should appear as well for heteronuclear systems (D'Incao and Esry, 2006a,b;Efimov, 1973aEfimov, , 1979Helfrich et al, 2010;Mikkelsen et al, 2015;Petrov and Werner, 2015;Wang et al, 2012dWang et al, , 2015b. In particular, in heteronuclear systems the mass-imbalanced nature of the threebody system preserves but modifies in an interesting way the discrete symmetry scaling characteristic of Efimov Figure 10 (Color online) (a)Schematic hyperspherical potential curve relevant to five-boson recombination when the twobody scattering length is negative, a < 0.…”
Section: H Efimov States In Heteronuclear Mass-imbalanced Systemsmentioning
confidence: 94%
“…The existence of an infinite series of three-body bound states for resonant two-body interaction, as predicted by Efimov (Efimov, 1970), is not only present for homonuclear systems, as such universal three-body bound states should appear as well for heteronuclear systems (D'Incao and Esry, 2006a,b;Efimov, 1973aEfimov, , 1979Helfrich et al, 2010;Mikkelsen et al, 2015;Petrov and Werner, 2015;Wang et al, 2012dWang et al, , 2015b. In particular, in heteronuclear systems the mass-imbalanced nature of the threebody system preserves but modifies in an interesting way the discrete symmetry scaling characteristic of Efimov Figure 10 (Color online) (a)Schematic hyperspherical potential curve relevant to five-boson recombination when the twobody scattering length is negative, a < 0.…”
Section: H Efimov States In Heteronuclear Mass-imbalanced Systemsmentioning
confidence: 94%
“…The resonance positions cannot be directly fitted from the experimental loss-rate data, since the excited resonance features are all already located into the unitarity limited regime, and, thus, effects of finite temperature would have to be included (for negative intraspecies scattering length, see Refs. [14,43,44]). Therefore, encouraged by the good agreement between the experimental findings and the vdW model, we extract Efimov resonance positions a (n) −,CsLi from the calculated trimer energy spectra as the average value of the two numerical grid points, between which the three-body states merge with the scattering continuum (see Fig.…”
Section: Csmentioning
confidence: 99%
“…In the following we compare our three-body recombination results with our theoretical model and with results obtained in 41 K-87 Rb and 40 K-87 Rb [28,29,31,53]. For negative scattering lengths, our theoretical framework [26] is applied, assuming no Efimov resonances as shown in Fig. 2 and 3.…”
mentioning
confidence: 95%
“…Mass-imbalanced systems can provide a much denser spectrum when all scattering lenghs are large [26,27]. So far only four different heteronuclear isotopic mixtures have been investigated.…”
mentioning
confidence: 99%