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腔极化激元的玻色玻璃相和超流相

Bose glass and superfluid phases of cavity polaritons.

作者信息

Malpuech G, Solnyshkov D D, Ouerdane H, Glazov M M, Shelykh I

机构信息

LASMEA, CNRS-Université Blaise Pascal, 24 Avenue des Landais, 63177 Aubière Cedex France.

出版信息

Phys Rev Lett. 2007 May 18;98(20):206402. doi: 10.1103/PhysRevLett.98.206402. Epub 2007 May 14.

Abstract

We report the calculation of cavity exciton-polariton phase diagram including realistic structural disorder. With increasing density polaritons first undergo a quasiphase transition toward a Bose glass: the condensate is localized in at least one minimum of the disorder potential. A further increase of the density leads to a percolation process of the polariton fluid giving rise to a Kosterlitz-Thouless phase transition toward superfluidity. The spatial representation of the condensate wave function as well as the spectrum of elementary excitations are obtained from the Gross-Pitaevskii equation for all the phases.

摘要

我们报告了包含实际结构无序的腔激子 - 极化激元相图的计算结果。随着密度增加,极化激元首先经历向玻色玻璃的准相变:凝聚体局域在无序势的至少一个极小值处。密度的进一步增加导致极化激元流体的渗流过程,从而引发向超流性的科斯特利茨 - Thouless相变。对于所有相,凝聚体波函数的空间表示以及元激发谱都是从格罗斯 - 皮塔耶夫斯基方程获得的。

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