Photorefractive Effects in Ferromagnetic Semiconductors with Superlattice Formed by Coherent Light Beams

A. Semchuk
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Abstract

Let us consider a wide-gap donor-type a ferromagnetic semiconductor (FMSC) with mean carrier density nOin the spin wave temperature range placed in an external constant electric field F→O//OZ, magnetic field H→O//F→O and variable weak magnetic field h→/H→O. Its face surface is subjected to several coherent light beams (CLBs), whose frequencies satisfe the inequality ε¯≪ℏω≪ε g (ε g is the energy-gap width). In this case, as a result of the interference phenomena, there appear new regularities in the character of the high-frequency CLB field influence on free carriers and magnons. Thus, for example, the spatial modulation of collision integrals and high-frequency light waves pressure force on electrons leads to the formation of superlattices of the carrier density, electron and magnon temperatures, electric field strength, and magnetization intensity in the system of non-equilibrium electrons and magnons of FMSC.
相干光束形成超晶格的铁磁半导体的光折变效应
我们考虑一种宽间隙给体型铁磁半导体(FMSC),其平均载流子密度在自旋波温度范围内为no1,置于恒定电场F→O// F→O、磁场H→O//F→O和可变弱磁场H→/H→O。它的表面受到若干相干光束(clb)的照射,这些光束的频率满足ε¯≪ω≪ε g (ε g是能隙宽度)的不等式。在这种情况下,由于干涉现象的存在,高频CLB场对自由载流子和磁振子的影响特性出现了新的规律。因此,例如,碰撞积分和高频光波对电子的压力的空间调制导致了FMSC非平衡电子和磁振子系统中载流子密度、电子和磁振子温度、电场强度和磁化强度的超晶格的形成。
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