A lattice theory for low energy fermions at finite chemical potential

Abstract

We construct a lattice theory describing a system of interacting nonrelativistic spin s=1/2 fermions at nonzero chemical potential. The theory is applicable whenever the interparticle separation is large compared to the range of the two-body potential, and does not suffer from a sign problem. In particular, the theory could be useful in studying the thermodynamic limit of fermion systems for which the scattering length is much larger than the interparticle spacing, with applications to realistic atomic systems and dilute neutron gases.

Revised introduction, several typos fixed. Conforms to version accepted for publication in Phys. Rev. Lett

References in corpus (3)

• Superfluid Fermi Gases with Large Scattering Length
• The singular inverse square potential, limit cycles and self-adjoint extensions
• Goldstone Bosons in the 3P2 Superfluid Phase of Neutron Matter and Neutrino Emission

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