Histories of adiabatic quantum transitions

M. Berry
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引用次数: 148

Abstract

The way in which the transition amplitude to an initially unoccupied state increases to its exponentially small final value is studied in detail in the adiabatic approximation, for a 2-state quantum system. By transforming to a series of superadiabatic bases, clinging ever closer to the exact evolving state, it is shown that transition histories renormalize onto a universal one, in which the amplitude grows to its final value as an error function (rather than via large oscillations as in the ordinary adiabatic basis). The time for the universal transition is of order √ (ћ/δ) where δ is the small adiabatic (slowness) parameter. In perturbation theory the pre-exponential factor of the final amplitude renormalizes superadiabatically from the incorrect value ⅓π (for the ordinary adiabatic basis) to the correct value unity. The various histories could be observed in spin experiments.
绝热量子跃迁的历史
在绝热近似下,对二态量子系统的跃迁振幅如何增加到其指数小的最终值进行了详细的研究。通过转换到一系列超绝热基,越来越接近于精确的演化状态,表明转变历史重新归一化为普遍的,其中振幅作为误差函数增长到其最终值(而不是通过普通绝热基中的大振荡)。普遍转变的时间为√(()/δ)阶,其中δ是小绝热(慢度)参数。在微扰理论中,最终振幅的指数前因子将超绝热从不正确的值1 / 3 π(对于普通绝热基)重新规格化到正确的值单位。在自旋实验中可以观察到不同的历史。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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