含半导体平面结构中非线性毫米波的产生

W. Hwang, D. Bolle
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引用次数: 0

摘要

本文研究了用非线性混频方法产生电磁波的问题。待分析结构如图1所示。它由不同的电介质层组成,其中一些可能是掺杂或未掺杂的砷化镓材料。它在中心平面上是对称的,在横向于法向〇和传播z方向上是无限均匀的。中心是单晶砷化镓材料薄层,具有光学非线性。非线性包括本征砷化镓材料的价电子和通过外部手段引入介质的传导电子的贡献。在中心层内传播的两个光波,由于光的混合,产生电偶极子分布,它们以输入波的和、差或谐波频率辐射电磁波。我们对差频波的产生特别感兴趣,对于两个CO2激光输入,差频波的范围为~ 150-4000 GHz。激发波的色散特性和场分布是由整个结构在该频率处的波导特性决定的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nonlinear MM wave generation in a planar structure containing semiconductor
In this paper we examine the problem of EM wave generation using nonlinear mixing schemes. The structure to be analyzed is shown in Fig. 1. It consists of layers of differing dielectrics, some of which may be doped or undoped GaAs materials. It is symmetric about the center plane and is infinite and uniform in the direction transverse to the normal ○ and the direction of propagation z. In the center is a thin layer of single crystal GaAs material which exhibits optical nonlinearity. The nonlinearity consists of the contributions from both the valence electrons of the intrinsic GaAs material and the conduction electrons introduced into the medium by external means. Two optical waves propagating inside the center layer induce, as a result of optical mixing, a distribution of electric dipoles which radiate EM waves at the sum, difference or harmonic frequencies of the input waves. We are particularly interested in the generation of waves at the difference frequency which, for two CO2 laser inputs, ranges from ∼150–4000 GHz. The dispersion characteristic and field distribution of the excited waves are determined by the waveguiding property of the whole structure at that frequency.
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