Plane- and stripe-wave phases of a spin-orbit-coupled Bose-Einstein condensate in an optical lattice with a Zeeman field

Kristian Mæland, Andreas T. G. Janssønn, Jonas H. Rygh, A. Sudbø
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引用次数: 4

Abstract

A weakly interacting, spin-orbit coupled, ultracold, dilute Bose gas on a two-dimensional square lattice with an external Zeeman field is studied. We explore the plane and stripe wave phases of the system involving nonzero condensate momenta, which occur when the Zeeman field is below a critical value. Their excitation spectra are found using Bogoliubov theory and by two different routes. The validity of each method to obtain the excitation spectrum is discussed, and it is found that projection on the lowest single-particle band is an excellent approximation in the plane wave phase, while it is a poor approximation in the stripe wave phase. While the plane wave phase has a phonon minimum at its single condensate momentum, revealing a nonzero sound velocity of the excitations, the stripe wave phase has quadratic minima at its two condensate momenta showing zero sound velocity of the excitations. We discuss how the presence of more than one condensate momentum is essential for these differences between the two phases.
具有塞曼场的光学晶格中自旋轨道耦合玻色-爱因斯坦凝聚体的平面波相位和条纹波相位
研究了具有外塞曼场的二维方形晶格上弱相互作用、自旋轨道耦合、超冷的稀玻色气体。我们研究了涉及非零凝聚动量的系统的平面波相位和条纹波相位,这发生在塞曼场低于临界值时。它们的激发谱是用Bogoliubov理论和两种不同的途径得到的。讨论了每种方法获得激发谱的有效性,发现在平面波相位,最低单粒子带上的投影是一个很好的近似,而在条纹波相位,它是一个很差的近似。平面波相在其单凝聚动量处声子最小值,表明激发态声子声速非零;条纹波相在其双凝聚动量处声子最小值为二次,表明激发态声速为零。我们讨论了一个以上的凝聚动量的存在对于两相之间的这些差异是如何必不可少的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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