Оптическое возбуждение спин-триплетных состояний двухэлектронных доноров в кремнии

В.В. Цыпленков, Р.Х. Жукавин, В.Н. Шастин
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Abstract

In this paper, we propose a method for resonant optical excitation of ortho states of two-electron donors in silicon, direct transitions to which from the ground state are extremely suppressed in case of a weak spin-orbit coupling. Excitation is proposed to be carried out using the points of anti-crossing of ortho and para states under conditions of uniaxial stress of the crystal. In these points the states cannot be unambiguously assigned to any group of states with a certain spin, as a result of which the optical transition becomes allowed. The structure of the energy levels of two-electron impurities is such that the excitation of such state almost unambiguously leads to the population of the underlying ortho-type state, which is expected to be very long-lived in the case of weak spin-orbit coupling. In the present work, theoretical estimates of the cross sections for optical transitions in the vicinity of the level anticrossing point as a function of strain for strong and weak spin-orbit coupling are made.
硅二电子供体自旋三倍状态的光激发
在本文中,我们提出了一种共振光学激发硅中双电子供体正位态的方法,在弱自旋-轨道耦合的情况下,从基态到正位态的直接跃迁被极大地抑制。提出在晶体的单轴应力条件下,利用正交准态的反交叉点进行激发。在这些点上,状态不能被明确地分配给具有一定自旋的任何一组状态,因此光学跃迁是允许的。双电子杂质的能级结构是这样的,这种态的激发几乎可以明确地导致底层正型态的居群,在弱自旋-轨道耦合的情况下,正型态的寿命预计会很长。本文从理论上估计了强自旋-轨道耦合和弱自旋-轨道耦合在水平反交叉点附近的光学跃迁截面与应变的关系。
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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