首页> 外文期刊>International Journal of Quantum Chemistry >THE EFFECTS OF STATIC QUARTIC ANHARMONICITY ON THE QUANTUM DYNAMICS OF A LINEAR OSCILLATOR WITH TIME-DEPENDENT HARMONIC FREQUENCY - PERTURBATIVE ANALYSIS AND NUMERICAL CALCULATIONS
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THE EFFECTS OF STATIC QUARTIC ANHARMONICITY ON THE QUANTUM DYNAMICS OF A LINEAR OSCILLATOR WITH TIME-DEPENDENT HARMONIC FREQUENCY - PERTURBATIVE ANALYSIS AND NUMERICAL CALCULATIONS

机译:静态四阶失谐对时滞谐波频率线性振荡子量子动力学的影响-微扰分析和数值计算

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The effects of quartic anharmonicity on the quantum dynamics of a linear oscillator with time-dependent force constant (K) or harmonic frequency (omega) are studied both perturbatively and numerically by the time-dependent Fourier grid Hamiltonian method. In the absence of anharmonicity, the ground-state population decreases and the population of an accessible excited state (k = 2,4,6...) increases with time. However, when anharmonicity is introduced, both the ground- and excited-state populations show typical oscillations. For weak coupling, the population of an accessible excited state at a certain instant of time (short) turns out to be a parabolic function of the anharmonic coupling constant (lambda), when all other parameters of the system are kept fixed. This parabolic nature of the excited-state population vs. the lambda profile is independent of the specific form of the time dependence of the force constant, K-f. However, it depends upon the rate at which K-t relaxes. For small anharmonic coupling strength and short time scales, the numerical results corroborate expectations based on the first-order time-dependent perturbative analysis, using a suitably repartitioned Hamiltonian that makes H-0 time-independent. Some of the possible experimental implications of our observations are analyzed, especially in relation to intensify oscillations observed in some charge-transfer spectra in systems in which the dephasing rates are comparable with the time scale of the electron transfer. (c) 1995 John Wiley and Sons, Inc. [References: 22]
机译:通过时变傅立叶网格哈密顿量法,以扰动和数值方式研究了四次非谐性对线性振荡器的动力学的影响,该线性振荡器具有随时间变化的力常数(K)或谐波频率(ω)。在不存在非谐性的情况下,基态种群随时间减少,可及的激发态种群(k = 2,4,6 ...)随时间增加。但是,当引入非谐性时,基态和激发态总体都显示出典型的振荡。对于弱耦合,当系统的所有其他参数保持固定时,在某个特定时刻(短)的可访问激发态的填充量将成为非谐波耦合常数(拉姆达)的抛物线函数。激发态总体相对于λ分布的抛物线性质与力常数K-f的时间依赖性的特定形式无关。但是,这取决于K-t的松弛速率。对于较小的非谐耦合强度和较短的时间尺度,数值结果证实了基于一阶时变扰动分析的期望,使用了经过适当重新划分的哈密顿量,使H-0与时间无关。分析了我们观察到的一些可能的实验含义,特别是在系统的某些电荷转移谱中观察到的振荡增强方面,在该系统中,相移速率与电子转移的时间尺度相当。 (c)1995年John Wiley and Sons,Inc. [参考:22]

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