Instability in multi-valley semiconductors in external electric and magnetic fields

IF 0.3 Q4 PHYSICS, MULTIDISCIPLINARY
E. R. Hasanov, Sh.G. Khalilova
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Abstract

It is theoretically proved that the excited wave in two-valley semiconductors is growing. It is indicated that the directions of external fields play an essential role for the appearance of growing waves in the sample. It is shown that oscillations can occur at certain values of the sample dimensions L ,L ,L x y z Analytical formulas for the frequency of the growing waves are obtained. The interval of variation of the external electric field in a strong magnetic field H c  has been determined. The paper takes into account that the time of transition from the lower valley to the upper valley differs from the time of transition from the upper valley to the lower valley. It means 12 21    In the sample, the total concentration is constant, and therefore, 0 ba =+= constnnn . The changes in the corresponding concentrations are equal to each other and have the opposite sign, i.e. nn ba  −=  . It is taken into account that at critical values of the electric and magnetic fields and the corresponding concentrations they change as a monochromatic wave. And the change in these quantities differs little from their equilibrium value. For simplicity of mathematical calculations, the external electric and magnetic fields are directed in the same way, i.e. in x direction. Since the current oscillations in one direction (for example, along x) are studied in the experiment, the following equalities were taken into account  = jj  zy = 0,0 . In the vicinity of the critical field at the beginning of the current oscillation in the sample, the current oscillation frequency is  10 += i ,  01 . In addition, the magnitude of the critical electric field, at which the current fluctuation changes depending on the magnetic field as follows 4 1 ~ external kr H E .
多谷半导体在外加电场和磁场下的不稳定性
从理论上证明了双谷半导体中的激发态波是不断增长的。结果表明,外场的方向对样品中生长波的出现起着至关重要的作用。结果表明,在样品尺寸L、L、L x y z的一定值下,振荡可以发生。确定了强磁场中外电场的变化间隔H c。本文考虑了从下谷到上谷的过渡时间与从上谷到下谷的过渡时间不同。表示12 21在样品中,总浓度是恒定的,因此0 ba =+= constnnn。相应的浓度变化相等,符号相反,即nn ba−=。考虑到在电场和磁场的临界值以及相应的浓度时,它们以单色波的形式变化。这些量的变化和它们的平衡值相差很小。为了数学计算的简单性,外部电场和磁场的方向是相同的,即在x方向。由于实验中研究的是电流沿一个方向(例如沿x方向)的振荡,因此考虑了以下等式= jjzy = 0,0。在样本中电流振荡开始时的关键场附近,电流振荡频率为: 01;此外,电流波动随磁场变化的临界电场的大小为4.1 ~外部kr H E。
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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来源期刊
自引率
50.00%
发文量
32
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