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Quantum-phase and information-entropy dynamics of a two-state molecular system interacting with strongly amplitude- and phase-squeezed fields

机译:与强振幅和相位压缩场相互作用的二态分子系统的量子相和信息熵动力学

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We perform numerically exact calculations of quantum dynamics for a two-state molecular model system interacting with initially single-mode strongly amplitude- and strongly phase-squeezed fields (average photon number [(n) over cap] = 8). The second-order correlation function for these fields are taken to be 2, which is equivalent to that for the chaotic field with the identical average photon number. Although the responses of the molecule for these two squeezed fields are relatively similar to those for the chaotic field as shown in a previous paper, there are found to be some significant differences among these fields in the dynamical behavior of quantum-phase distributions of photons, i.e., the Pegg-Barnett phase and the Q function distributions. These differences are also elucidated by the dynamics of the information entropy for the molecule, i.e., molecular entropy, which represents the degree of entanglement between the molecule and the photon field. (C) 2000 American Institute of Physics. [S0021-9606(00)00406-2]. [References: 29]
机译:我们对与初始单模强振幅和强相位压缩场(平均光子数[[n]上限)[= 8])相互作用的二态分子模型系统进行量子动力学的精确数值计算。这些场的二阶相关函数取为2,它等于具有相同平均光子数的混沌场的二阶相关函数。尽管分子对这两个压缩场的响应与先前论文中对混沌场的响应相对相似,但发现这些场在光子量子相分布的动力学行为方面存在一些显着差异,即Pegg-Barnett相位和Q函数分布。这些差异还通过分子信息熵的动力学来阐明,即分子熵代表分子与光子场之间的缠结程度。 (C)2000美国物理研究所。 [S0021-9606(00)00406-2]。 [参考:29]

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