Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice

A low-energy theory of the Nambu-Goldstone excitation spectrum and the corresponding speed of sound of an interacting Fermi mixture of Lithium-6 and Potassium-40 atoms in a two-dimensional optical lattice at finite temperatures with the Fulde-Ferrell order parameter has been formulated. It is assume...

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Main Author: Z. G. Koinov
Format: Article
Language:English
Published: Hindawi Limited 2015-01-01
Series:Advances in Condensed Matter Physics
Online Access:http://dx.doi.org/10.1155/2015/952852
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spelling doaj-7ee958bfcc7f46bc971d661cbb82515c2020-11-24T23:53:17ZengHindawi LimitedAdvances in Condensed Matter Physics1687-81081687-81242015-01-01201510.1155/2015/952852952852Collective Modes of an Ultracold 6Li-40K Mixture in an Optical LatticeZ. G. Koinov0Department of Physics and Astronomy, University of Texas at San Antonio, San Antonio, TX 78249, USAA low-energy theory of the Nambu-Goldstone excitation spectrum and the corresponding speed of sound of an interacting Fermi mixture of Lithium-6 and Potassium-40 atoms in a two-dimensional optical lattice at finite temperatures with the Fulde-Ferrell order parameter has been formulated. It is assumed that the two-species interacting Fermi gas is described by the one-band Hubbard Hamiltonian with an attractive on-site interaction. The discussion is restricted to the BCS side of the Feshbach resonance where the Fermi atoms exhibit superfluidity. The quartic on-site interaction is decoupled via a Hubbard-Stratonovich transformation by introducing a four-component boson field which mediates the Hubbard interaction. A functional integral technique and a Legendre transform are used to give a systematic derivation of the Schwinger-Dyson equations for the generalized single-particle Green’s function and the Bethe-Salpeter equation for the two-particle Green’s function and the associated collective modes. The numerical solution of the Bethe-Salpeter equation in the generalized random phase approximation shows that there exist two distinct sound velocities in the long-wavelength limit. In addition to low-energy (Goldstone) mode, the two-species Fermi gas has a superfluid phase revealed by two roton-like minima in the asymmetric collective-mode energy.http://dx.doi.org/10.1155/2015/952852
collection DOAJ
language English
format Article
sources DOAJ
author Z. G. Koinov
spellingShingle Z. G. Koinov
Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
Advances in Condensed Matter Physics
author_facet Z. G. Koinov
author_sort Z. G. Koinov
title Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
title_short Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
title_full Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
title_fullStr Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
title_full_unstemmed Collective Modes of an Ultracold 6Li-40K Mixture in an Optical Lattice
title_sort collective modes of an ultracold 6li-40k mixture in an optical lattice
publisher Hindawi Limited
series Advances in Condensed Matter Physics
issn 1687-8108
1687-8124
publishDate 2015-01-01
description A low-energy theory of the Nambu-Goldstone excitation spectrum and the corresponding speed of sound of an interacting Fermi mixture of Lithium-6 and Potassium-40 atoms in a two-dimensional optical lattice at finite temperatures with the Fulde-Ferrell order parameter has been formulated. It is assumed that the two-species interacting Fermi gas is described by the one-band Hubbard Hamiltonian with an attractive on-site interaction. The discussion is restricted to the BCS side of the Feshbach resonance where the Fermi atoms exhibit superfluidity. The quartic on-site interaction is decoupled via a Hubbard-Stratonovich transformation by introducing a four-component boson field which mediates the Hubbard interaction. A functional integral technique and a Legendre transform are used to give a systematic derivation of the Schwinger-Dyson equations for the generalized single-particle Green’s function and the Bethe-Salpeter equation for the two-particle Green’s function and the associated collective modes. The numerical solution of the Bethe-Salpeter equation in the generalized random phase approximation shows that there exist two distinct sound velocities in the long-wavelength limit. In addition to low-energy (Goldstone) mode, the two-species Fermi gas has a superfluid phase revealed by two roton-like minima in the asymmetric collective-mode energy.
url http://dx.doi.org/10.1155/2015/952852
work_keys_str_mv AT zgkoinov collectivemodesofanultracold6li40kmixtureinanopticallattice
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