Density Functional Theory for non-relativistic Fermions in the Unitarity Limit

dc.creatorRupak, Gautam
dc.creatorSchaefer, Thomas
dc.date2008-04-17
dc.date2008-11-17
dc.date.accessioned2026-07-07T12:55:04Z
dc.date.available2026-07-07T12:55:04Z
dc.descriptionWe derive an energy density functional for non-relativistic spin one-half fermions in the limit of a divergent two-body scattering length. Using an epsilon expansion around d=4-epsilon spatial dimensions we compute the coefficient of the leading correction beyond the local density approximation (LDA). In the case of N fermionic atoms trapped in a harmonic potential this correction has the form E=E_(LDA)(1+c_s (3N)^(-2/3)), where E_(LDA) is the total energy in LDA approximation. At next-to-leading order in the epsilon expansion we find c_s=1.68, which is significantly larger than the result for non-interacting fermions, c_s=0.5.
dc.description17 pages, final version, Nuclear Physics A, in press
dc.identifierhttps://arxiv.org/abs/0804.2678
dc.identifierhttp://arxiv.org/abs/0804.2678
dc.identifierNucl.Phys.A816:52-64,2009
dc.identifierdoi:10.1016/j.nuclphysa.2008.11.004
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/224148
dc.subjectNuclear Theory
dc.subjectOther Condensed Matter
dc.titleDensity Functional Theory for non-relativistic Fermions in the Unitarity Limit
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