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Nuclear Physics A

Three-Body Recombination in Atoms with Large Scattering Length

Eric Braaten

Published Jun 1, 2007• 0 citations
Publisher
DOI
10.1016/j.nuclphysa.2007.03.125

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For atoms with large scattering length, the dependence of the three-body recombination rate on the collision energy is determined by the scattering length and the Efimov three-body parameters and can be expressed in terms of universal functions of a single scaling variable. We use published results on the three-body recombination rate for 4He^{4}\mathrm{He}4He atoms to constrain the universal functions. We then use those universal functions to calculate the three-body recombination rate for other atoms with large scattering length at nonzero temperature. The constraints from the 4He^{4}\mathrm{He}4He results are strong if the scattering length is near the minimum of the three-body recombination rate at threshold. We apply our results to 133Cs^{133}\mathrm{Cs}133Cs atoms with a large positive scattering length, and compare them with experimental results from the Innsbruck group.
We demonstrate the implications of Efimov physics in the recently measured recombination rate of 133Cs^{133}\mathrm{Cs}133Cs atoms. By employing previously calculated results for the energy dependence of the recombination rate of 4He^{4}\mathrm{He}4He atoms, we obtain three independent scaling functions that are capable of describing the recombination rates over a large energy range for identical bosons with large scattering length. We benchmark these and previously obtained scaling functions by successfully comparing their predictions with full atom-dimer phase shift calculations with artificial 4He^{4}\mathrm{He}4He potentials yielding large scattering lengths. Exploiting universality, we finally use these functions to determine the three-body recombination rate of 133Cs^{133}\mathrm{Cs}133Cs atoms with large positive scattering length, compare our results to experimental data obtained by Kraemer et al. at Innsbruck and find excellent agreement.