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Resonant second harmonics generation of the submillimeter surface wave in the semiconductor superlattice bounded by a metal

机译:以金属为界的半导体超晶格中亚毫米波表面波的共振二次谐波产生

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In the present paper we are interested in compositional superlattices of the first kind with periodically alternating layers of wide-band and narrow-band semiconductors, where the formation of conductive two-dimensional conductive layers takes place due to a significant distortion of the energy band structure. The superlattices based on GaAs-AlGaAs heterostructures can be taken as an example in this case. In the presence of the external quantizing magnetic field, the realisation of the quantum Hall effect (QHE) in two-dimensional conductive layers is possible. In the present paper we deal with the surface magnetoplasma modes propagating on the lateral surface (i.e. on the surface which is perpendicular to two-dimensional conductive layers and is parallel to the superlattice axis) of the semiconductor superlattice coated by a metal plane. Here we study the process of the resonant second harmonics generation of the SM, which can be of interest for design of semiconductor frequency multipliers. The resonant second harmonics generation is realised when the eigenfrequencies and the wavenumbers of the first and the second harmonics are coupled by phase synchronism conditions.
机译:在本文中,我们对具有宽带半导体和窄带半导体的周期性交替层的第一类超晶格感兴趣,其中由于能带结构的明显变形而形成了导电二维导电层。在这种情况下,可以以基于GaAs-AlGaAs异质结构的超晶格为例。在存在外部量化磁场的情况下,可以在二维导电层中实现量子霍尔效应(QHE)。在本文中,我们处理了在由金属平面覆盖的半导体超晶格的侧面(即,垂直于二维导电层并且平行于超晶格轴的表面)上传播的表面磁等离子体模式。在这里,我们研究SM的谐振二次谐波的产生过程,这对于半导体倍频器的设计可能是有意义的。当第一和第二谐波的本征频率和波数通过相位同步条件耦合时,实现了谐振第二谐波的产生。

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