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被困于光学晶格中的超冷费米子原子中粒子-空穴对的玻色-爱因斯坦凝聚。

Bose-Einstein condensation of particle-hole pairs in ultracold fermionic atoms trapped within optical lattices.

作者信息

Lee Chaohong

机构信息

Max Planck Institute for the Physics of Complex Systems, Nöthnitzer Strasse 38, D-01187 Dresden, Germany.

出版信息

Phys Rev Lett. 2004 Sep 17;93(12):120406. doi: 10.1103/PhysRevLett.93.120406. Epub 2004 Sep 14.

Abstract

We investigate the Bose-Einstein condensation (BEC, superfluidity) of particle-hole pairs in ultracold fermionic atoms with repulsive interactions and arbitrary polarization, which are trapped within optical lattices. In the strongly repulsive limit, the dynamics of particle-hole pairs can be described by a hard-core Bose-Hubbard model. The insulator-superfluid and charge-density-wave- (CDW) superfluid phase transitions can be induced by decreasing and increasing the potential depths with controlling the trapping laser intensity, respectively. The parameter and polarization dependence of the critical temperatures for the ordered states (BEC and/or CDW) are discussed simultaneously.

摘要

我们研究了被困在光学晶格中的具有排斥相互作用和任意极化的超冷费米子原子中粒子-空穴对的玻色-爱因斯坦凝聚(BEC,超流性)。在强排斥极限下,粒子-空穴对的动力学可以用硬核玻色-哈伯德模型来描述。通过分别控制俘获激光强度来降低和增加势阱深度,可以诱导绝缘体-超流和电荷密度波(CDW)超流相变。同时讨论了有序态(BEC和/或CDW)临界温度的参数和极化依赖性。

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