振幅双稳态中的量子跃迁:追踪相干和可逆的状态定位

Th. K. Mavrogordatos
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引用次数: 0

摘要

我们研究了开放驱动杰恩斯-康明斯模型中光的宏观可变态之间发生的量子跃迁的性质。我们发现,在[H. J. Carmichael, Phys. Rev. X 5, 031028 (2015)]中考虑的零自发辐射极限下,从高光子态到真空态的跃迁包含两个阶段。第一部分是相干的,以量子轨迹理论预测的空测量记录为例,以状态叠加的局部化为模型。底层演化由不稳定态(通常分裂为复合态)介导,不稳定态由条件密度矩阵和相应的空腔场等概率分布确定。不稳定态随后衰减到真空,完成跃迁。定位中的相干性允许将空测量光子平均值反转为初始值,以解释通常只占空腔寿命一小部分的完全切换。这种机制与双稳态信号中从真空到高光子态的跃迁形成鲜明对比。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum jumps in amplitude bistability: tracking a coherent and invertible state localization
We investigate the nature of quantum jumps occurring between macroscopic metastable states of light in the open driven Jaynes-Cummings model. We find that, in the limit of zero spontaneous emission considered in [H. J. Carmichael, Phys. Rev. X 5, 031028 (2015)], the jumps from a high-photon state to the vacuum state entail two stages. The first part is coherent and modelled by the localization of a state superposition, in the example of a null-measurement record predicted by quantum trajectory theory. The underlying evolution is mediated by an unstable state (which often splits to a complex of states), identified by the conditioned density matrix and the corresponding quasiprobability distribution of the cavity field. The unstable state subsequently decays to the vacuum to complete the jump. Coherence in the localization allows for inverting the null-measurement photon average about its initial value, to account for the full switch which typically lasts a small fraction of the cavity lifetime. This mechanism is contrasted to the jumps leading from the vacuum to the high-photon state in the bistable signal. Spontaneous emission degrades coherence in the localization, and prolongs the jumps.
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