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Bethe-Salpeter equations for the collective-mode spectrum of a superfluid Fermi gas in a moving optical lattice

机译:一个集体模式谱的Bethe-salpeter方程   流体光学晶格中的超流体费米气体

摘要

We derive the Bethe-Salpeter (BS) equations for the collective-mode spectrumof superfluid Fermi gases of equal mixture of atomic Fermi gas of two hyperfinestates loaded into a moving optical lattice. In a moving lattice the superfluidstate is unstable due to spontaneous emission of the short-wavelength rotonlikeexcitations which appear in the spectrum of the collective modes. It is shownthat the spectrum obtained by the BS equations is in an excellent agreementwith the collective-mode dispersion calculated by the perturbation approach,while there are some differences between the results obtained by densityresponse function method and by the BS approach. The difference increases withincreasing the lattice velocity, which can be seen in the analyticalapproximations for the dispersion relation in the long-wavelength limit in aweak-coupling regime.
机译:我们推导了Bethe-Salpeter(BS)方程,该方程是加载到移动光学晶格中的两个超精细状态的原子费米气体的均等混合的超流体费米气体的集体模式谱。在运动晶格中,由于出现在集体模态谱中的短波rotonlike激发的自发发射,超流体状态不稳定。结果表明,由BS方程获得的光谱与通过扰动方法计算出的集体模式色散非常吻合,而通过密度响应函数法获得的结果与通过BS方法获得的结果之间存在一些差异。差异随着晶格速度的增加而增加,这可以从弱耦合状态下长波长极限中的色散关系的解析近似中看出。

著录项

  • 作者

    Koinov, Zlatko;

  • 作者单位
  • 年度 2010
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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