具有“最小噪声”的时变量子阻尼振荡器:应用于非理想腔中的非平稳卡西米尔效应

V. Dodonov
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引用次数: 12

摘要

在具有两个非交换delta相关噪声算子的Heisenberg-Langevin方程框架中,我们考虑了具有任意时变频率和阻尼系数的量子阻尼谐振子的一致模型。对于与阻尼系数具有相同时间依赖性的“最小噪声”相关函数集,我们得到了精确解,这是对无阻尼非平稳振荡器的Husimi解的推广。将该模型应用于具有周期时变电导率的半导体薄边界层腔内的非稳态卡西米尔效应引起的真空或热态光子产生问题,模拟了壁的周期性位移。得到了存在耗散的共振条件下光子产生速率的一般公式。
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Time-dependent quantum damped oscillator with ‘minimal noise’: application to the nonstationary Casimir effect in nonideal cavities
We consider a consistent model of a quantum damped harmonic oscillator with arbitrary time-dependent frequency and damping coefficients in the frameworks of the Heisenberg–Langevin equations with two noncommuting delta-correlated noise operators. For the 'minimal noise' set of correlation functions, which have the same time dependence as the damping coefficient, we obtain the exact solution, which is the generalization of Husimi's solution for the undamped nonstationary oscillator. The model is applied to the problem of the photon creation from vacuum or thermal states due to the nonstationary Casimir effect inside the cavity with periodical time-dependent conductivity of the thin semiconductor boundary layer, simulating the periodical displacements of the wall. The general formula for the rate of photon generation under the resonance conditions in the presence of dissipation is obtained.
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