强电场中李-诺顿-勒贝德角效应的量子理论

Andrei G. Lebed
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引用次数: 0

摘要

不久前,小林等人通过实验研究了强电场中所谓的李-诺顿-勒贝德(LNL)角效应[Kobayashi, K.; Saito, M.; Omichi E.; Osada, T. Phys. Rev. Lett. 2006, 96, 126601]。他们发现在基于 α-(ET)2 的有机导体中,强电场会分割 LNL 的最大电导率,并假设性地引入了相应的电导率方程。本文首次提出了中强电场中 LNL 角振荡的量子力学理论。我们特别证明,我们所得到的近似理论公式很好地描述了上述实验。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum Theory of Lee–Naughton–Lebed’s Angular Effect in Strong Electric Fields
Some time ago, Kobayashi et al. experimentally studied the so-called Lee–Naughton–Lebed’s (LNL) angular effect in strong electric fields [Kobayashi, K.; Saito, M.; Omichi E.; Osada, T. Phys. Rev. Lett. 2006, 96, 126601]. They found that strong electric fields split the LNL conductivity maxima in an α-(ET)2-based organic conductor and hypothetically introduced the corresponding equation for conductivity. In this paper, for the first time, we suggest the quantum mechanical theory of the LNL angular oscillations in moderately strong electric fields. In particular, we demonstrate that the approximate theoretical formula obtained by us well describes the above mentioned experiments.
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