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Energetics of a strongly correlated Fermi gas

Journal Article · · Annals of Physics (New York)
 [1]
  1. Institute for Nuclear Theory, University of Washington, Seattle, WA 98195-1550 (United States)
The energy of the two-component Fermi gas with the s-wave contact interaction is a simple linear functional of its momentum distribution: E{sub internal}=h{sup 2}{omega}C/4{pi}am+{sigma}{sub k{sigma}}(h{sup 2}k{sup 2}/2m)(n{sub k{sigma}}= -C/k{sup 4}) where the external potential energy is not included, a is the scattering length, {omega} is the volume, n{sub k{sigma}} is the average number of fermions with wave vector k and spin {sigma}, and C{identical_to}lim{sub k{yields}}{sub {infinity}}k{sup 4}n{sub k{up_arrow}}=lim{sub k{yields}}{sub {infinity}}k{sup 4}n{sub k{down_arrow}}. This result is a universal identity. Its proof is facilitated by a novel mathematical idea, which might be of utility in dealing with ultraviolet divergences in quantum field theories. Other properties of this Fermi system, including pair correlations and the dimer-fermion scattering length, are also studied.
OSTI ID:
21167680
Journal Information:
Annals of Physics (New York), Journal Name: Annals of Physics (New York) Journal Issue: 12 Vol. 323; ISSN 0003-4916; ISSN APNYA6
Country of Publication:
United States
Language:
English

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