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 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 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 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 atoms. By employing previously calculated results for the energy dependence of the recombination rate of
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 potentials yielding large scattering lengths. Exploiting universality, we finally use these functions to determine the three-body recombination rate of
133Cs atoms with large positive scattering length, compare our results to experimental data obtained by Kraemer et al. at Innsbruck and find excellent agreement.