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Quantum dynamics of interacting excitonic-vibronic dimer

机译:相互作用的激子-振动子二聚体的量子动力学

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摘要

A carrier on a symmetric dimer with a weak hopping integral, interacting (via a site-local coupling) strongly with on-site oscillators is considered. It is shown that the dynamics of the low excited nonstationary states is, owing to strong carrier-oscillator correlations, incompatible with that of the nonlinear Liouville equation theory. The oscillators are, owing to carrier-oscillator correlations, fully relaxed to the instantaneous rather than to the mean carrier position and need no time-delay or relaxation mechanism to respond to the shifted carrier's position, in contrast to the usual Holstein and Davydov picture. The origin of the standard Debye-Waller renormalization is scrutinized using the Tokuyama-Mori theory including all the excited states of the oscillators and rigorous statements are made concerning its form. Limitations on the time interval of applicability of the semiclassical description resulting from the carrier dynamics are discussed.
机译:考虑了对称二聚体上具有弱跳跃积分的载波,该载波具有与现场振荡器强烈的相互作用(通过局部-局部耦合)。结果表明,由于强的载流子相关性,低激发态非平稳态的动力学与非线性Liouville方程理论不相容。与通常的Holstein和Davydov图像相反,由于载波-振荡器的相关性,振荡器对瞬时位置完全放松,而不是对平均载波位置完全放松,并且不需要时延或松弛机制来响应移位后的载波位置。标准德比-华勒重归一化的起源使用德山-森理论(包括德州仪器所有振子的激发态)进行了仔细审查,并对其形式作了严格的表述。讨论了由于载流子动力学而导致的半经典描述适用时间间隔的限制。

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