Threshold singularities in a Fermi gas with attractive potential in one dimension

We consider the one-dimensional gas of fermions with spin S interacting via an attractive δ-function potential using the Bethe Ansatz solution. In zero magnetic field the atoms form bound states of N=2S+1 fermions, i.e. generalized Cooper states with each atom having a different spin component. For...

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Main Authors: P. Schlottmann, A.A. Zvyagin
Format: Article
Language:English
Published: Elsevier 2015-03-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321315000127
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spelling doaj-5d0cdd76054c49eea40fe85df21ca47e2020-11-24T23:44:10ZengElsevierNuclear Physics B0550-32132015-03-01892269287Threshold singularities in a Fermi gas with attractive potential in one dimensionP. Schlottmann0A.A. Zvyagin1Department of Physics, Florida State University, Tallahassee, FL 32306, USAB.I. Verkin Institute for Low Temperature Physics and Engineering, Ukrainian National Academy of Sciences, 47 Lenin Avenue, Kharkov, 61103, Ukraine; Max-Planck-Institut für Physik komplexer Systeme, D-01187, Dresden, GermanyWe consider the one-dimensional gas of fermions with spin S interacting via an attractive δ-function potential using the Bethe Ansatz solution. In zero magnetic field the atoms form bound states of N=2S+1 fermions, i.e. generalized Cooper states with each atom having a different spin component. For low energy excitations the system is a Luttinger liquid and is properly described by a conformal field theory with conformal charge c=1. The linear dispersion of a Luttinger liquid is asymptotically exact in the low-energy limit where the band curvature terms in the dispersion are irrelevant. For higher energy excitations, however, the spectral function displays deviations in the neighborhood of the single-particle (hole) energy, which can be described by an effective X-ray edge type model. Using the Bethe Ansatz solution we obtain expressions for the critical exponents for the single-particle (hole) Green's function. This model can be relevant in the context of ultracold atoms with effective total spin S confined to an elongated optical trap.http://www.sciencedirect.com/science/article/pii/S0550321315000127
collection DOAJ
language English
format Article
sources DOAJ
author P. Schlottmann
A.A. Zvyagin
spellingShingle P. Schlottmann
A.A. Zvyagin
Threshold singularities in a Fermi gas with attractive potential in one dimension
Nuclear Physics B
author_facet P. Schlottmann
A.A. Zvyagin
author_sort P. Schlottmann
title Threshold singularities in a Fermi gas with attractive potential in one dimension
title_short Threshold singularities in a Fermi gas with attractive potential in one dimension
title_full Threshold singularities in a Fermi gas with attractive potential in one dimension
title_fullStr Threshold singularities in a Fermi gas with attractive potential in one dimension
title_full_unstemmed Threshold singularities in a Fermi gas with attractive potential in one dimension
title_sort threshold singularities in a fermi gas with attractive potential in one dimension
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2015-03-01
description We consider the one-dimensional gas of fermions with spin S interacting via an attractive δ-function potential using the Bethe Ansatz solution. In zero magnetic field the atoms form bound states of N=2S+1 fermions, i.e. generalized Cooper states with each atom having a different spin component. For low energy excitations the system is a Luttinger liquid and is properly described by a conformal field theory with conformal charge c=1. The linear dispersion of a Luttinger liquid is asymptotically exact in the low-energy limit where the band curvature terms in the dispersion are irrelevant. For higher energy excitations, however, the spectral function displays deviations in the neighborhood of the single-particle (hole) energy, which can be described by an effective X-ray edge type model. Using the Bethe Ansatz solution we obtain expressions for the critical exponents for the single-particle (hole) Green's function. This model can be relevant in the context of ultracold atoms with effective total spin S confined to an elongated optical trap.
url http://www.sciencedirect.com/science/article/pii/S0550321315000127
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