Phys. Rev. A 76, 013615 (2007) [5 pages]
Stability of spinor Fermi gases in tight waveguides
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Citing Articles
A. del Campo, 1 J. G. Muga, 1 and M. D. Girardeau21Departamento de Química-Física, Universidad del País Vasco, Apartado 644, 48080 Bilbao, Spain
2College of Optical Sciences, University of Arizona, Tucson, Arizona 85721, USA
Received 8 May 2007; published 17 July 2007
The two- and three-body correlation functions of the ground state of an optically trapped ultracold spin- Fermi gas (SFG) in a tight waveguide [one-dimensional (1D) regime] are calculated in the plane of even- and odd-wave coupling constants, assuming a 1D attractive zero-range odd-wave interaction induced by a 3D p-wave Feshbach resonance, as well as the usual repulsive zero-range even-wave interaction stemming from 3D s-wave scattering. The calculations are based on the exact mapping from the SFG to a “Lieb-Liniger-Heisenberg” model with delta-function repulsions depending on isotropic Heisenberg spin-spin interactions, and indicate that the SFG should be stable against three-body recombination in a large region of the coupling constant plane encompassing parts of both the ferromagnetic and antiferromagnetic phases. However, the limiting case of the fermionic Tonks-Girardeau gas, a spin-aligned 1D Fermi gas with infinitely attractive p-wave interactions, is unstable in this sense. Effects due to the dipolar interaction and a Zeeman term due to a resonance-generating magnetic field do not lead to shrinkage of the region of stability of the SFG.
©2007 The American Physical Society
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