动态极化梯度场中的自旋和密度自序

N. Masalaeva, W. Niedenzu, F. Mivehvar, H. Ritsch
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引用次数: 6

摘要

研究了光学腔中双组分玻色-爱因斯坦凝聚体的零温度量子相图。两个原子自旋态是拉曼耦合的两个横向正交极化,蓝色失谐平面波激光产生排斥腔势。对于弱泵浦,激光倾向于具有均匀密度和预定的均匀自旋方向的状态。当一个泵浦激光器的偏振方向与腔模偏振方向平行时,相干散射到谐振腔内的光子会沿腔轴产生偏振梯度,从而产生远程密度-密度、自旋-密度和自旋-自旋相互作用。我们证明了耦合原子-腔系统实现了具有丰富相图的$t$-$J$-$V$-$W$模型的核心方面。在平均场极限下,我们确定了至少四个定性不同的密度有序相和自旋有序相,包括沿腔轴的铁磁有序相和反铁磁有序相,这可以通过泵浦强度和失谐来控制。发射场的振幅和相位的无损观测具有实现相位的强特征,并允许实时观察潜在的动力学。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spin and density self-ordering in dynamic polarization gradients fields
We study the zero-temperature quantum phase diagram for a two-component Bose-Einstein condensate in an optical cavity. The two atomic spin states are Raman coupled by two transverse orthogonally-polarized, blue detuned plane-wave lasers inducing a repulsive cavity potential. For weak pump the lasers favor a state with homogeneous density and predefined uniform spin direction. When one pump laser is polarized parallel to the cavity mode polarization, the photons coherently scattered into the resonator induce a polarization gradient along the cavity axis, which mediates long-range density-density, spin-density, and spin-spin interactions. We show that the coupled atom-cavity system implements central aspects of the $t$-$J$-$V$-$W$ model with a rich phase diagram. At the mean-field limit we identify at least four qualitatively distinct density- and spin-ordered phases including ferro- and anti-ferromagnetic order along the cavity axis, which can be controlled via the pump strength and detunings. Nondestructive observation of amplitude and phase of the emitted fields bears strong signatures of the realized phase and allows for real-time observation of the underlying dynamics.
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