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arXiv 1709.08646cond-mat.quant-gas
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集体原子衰变耗散Dicke模型:双稳态、噪声驱动激活和非热一级超辐射跃迁

Dissipative Dicke Model with Collective Atomic Decay: Bistability, Noise-Driven Activation and Non-Thermal First Order Superradiance Transition

Jan Gelhausen, Michael Buchhold

摘要:

Dicke模型描述了激光驱动的二能级原子系综与量子化光场的相干相互作用。它是在腔QED实验中实现的,除了相干Dicke动力学特征之外,还由于例如原子自发发射和腔光子损失而耗散。自发发射支持单个原子激发的不相关衰减以及由$N$原子共享的激发的增强的集体衰减,并且其强度由腔几何形状确定。基于Heisenberg-Langevin方程和随机Bloch方程,导出了包含两个自发发射通道的耗散Dicke模型的多体主方程,并分析了其动力学性质.我们发现,集体损失通道导致的区域之间的空和超辐射态的双稳态。这些状态之间的跃迁是由非热的马尔可夫噪声驱动的。耗散和相干元素之间的相互作用导致了一个真正的非平衡态动力学的非平衡状态,这是通过一个非保守力和乘法噪声核随机布洛赫方程中出现的。本文提出了一种基于随机非线性光学Bloch方程的半经典方法,该方法对无限程Dicke模型在大$N$极限下是精确的.一个有效的自由能功能的情况下,然而,有必要包括波动修正与$\mathcal{O}(1/N)$有限的$N<\infty$定位之间的超辐射和空腔的非热的一阶相变。

英文摘要:

The Dicke model describes the coherent interaction of a laser-driven ensemble of two level atoms with a quantized light field. It is realized within cavity QED experiments, which in addition to the coherent Dicke dynamics feature dissipation due to e.g. atomic spontaneous emission and cavity photon loss. Spontaneous emission supports the uncorrelated decay of individual atomic excitations as well as the enhanced, collective decay of an excitation that is shared by $N$ atoms and whose strength is determined by the cavity geometry. We derive a many-body master equation for the dissipative Dicke model including both spontaneous emission channels and analyze its dynamics on the basis of Heisenberg-Langevin and stochastic Bloch equations. We find that the collective loss channel leads to a region of bistability between the empty and the superradiant state. Transitions between these states are driven by non-thermal, markovian noise. The interplay between dissipative and coherent elements leads to a genuine non-equilibrium dynamics in the bistable regime, which is expressed via a non-conservative force and a multiplicative noise kernel appearing in the stochastic Bloch equations. We present a semiclassical approach, based on stochastic nonlinear optical Bloch equations, which for the infinite-range Dicke Model become exact in the large-$N$-limit. The absence of an effective free energy functional, however, necessitates to include fluctuation corrections with $\mathcal{O}(1/N)$ for finite $N<\infty$ to locate the non-thermal first-order phase transition between the superradiant and the empty cavity.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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