The scattering amplitude of ultracold atoms near the p-wave magnetic Feshbach Resonance
arXiv:1010.0293 · doi:10.1103/PhysRevA.82.062712
Abstract
Most of the current theories on the p-wave superfluid in cold atomic gases are based on the effective-range theory for the two-body scattering, where the low energy p-wave scattering amplitude is given by , where is the incident momentum, and and are the -independent scattering volume and effective-range, respectively. However, due to the long-range nature of the van der Waals interaction between two colliding ultracold atoms, the p-wave scattering amplitude of the two atoms is not described by the effective-range theory. In this paper we provide an explicit calculation for the p-wave scattering of two ultracold atoms near the p-wave magnetic Feshbach resonance (PMFR). We show that the low energy p-wave scattering amplitude in the presence of PMFR takes the form $f_1(k)=-1/[ik+1/(\mathcal{V}^{\mathrm{eff}}k^2)+1/(\mathcal{S}^{\mathrm{eff}%}k)+1/\mathcal{R}^{\mathrm{eff}}]$ where and are % -dependent parameters. Based on this result, we show sufficient conditions for the effective range theory to be a good approximation of the exact scattering amplitude. Using these conditions we show that the effective-range theory is a good approximation for the p-wave scattering in the ultracold gases of Li and K when the scattering volume is enhanced by the resonance.
13 pages, 3 figs
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