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A Theoretical Treatment of THz Resonances in Semiconductor GaAs p–n Junctions

机译:半导体GaAs p–n结中THz共振的理论处理

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摘要

Semiconductor heterostructures are suitable for the design and fabrication of terahertz (THz) plasmonic devices, due to their matching carrier densities. The classical dispersion relations in the current literature are derived for metal plasmonic materials, such as gold and silver, for which a homogeneous dielectric function is valid. Penetration of the electric fields into semiconductors induces locally varying charge densities and a spatially varying dielectric function is expected. While such an occurrence renders tunable THz plasmonics a possibility, it is crucial to understand the conditions under which propagating resonant conditions for the carriers occur, upon incidence of an electromagnetic radiation. In this manuscript, we derive a dispersion relation for a p–n heterojunction and apply the methodology to a GaAs p–n junction, a material of interest for optoelectronic devices. Considering symmetrically doped p- and n-type regions with equal width, the effect of certain parameters (such as doping and voltage bias) on the dispersion curve of the p–n heterojunction were investigated. Keeping in sight the different effective masses and mobilities of the carriers, we were able to obtain the conditions that yield identical dielectric functions for the p- and n-regions. Our results indicated that the p–n GaAs system can sustain propagating resonances and can be used as a layered plasmonic waveguide. The conditions under which this is feasible fall in the frequency region between the transverse optical phonon resonance of GaAs and the traditional cut-off frequency of the diode waveguide. In addition, our results indicated when the excitation was slightly above the phonon resonance frequency, the plasmon propagation attained low-loss characteristics. We also showed that the existence or nonexistence of the depletion zone between the p- and n- interfaces allowed certain plasmon modes to propagate, while others decayed rapidly, pointing out the possibility for a design of selective filters.
机译:半导体异质结构由于其匹配的载流子密度而适合于太赫兹(THz)等离子体器件的设计和制造。当前文献中的经典色散关系是针对金属等离激元材料(例如金和银)得出的,其均质介电函数是有效的。电场渗透到半导体中会引起局部变化的电荷密度,并且期望空间变化的介电功能。尽管这种情况使可调的THz等离子体激元成为可能,但至关重要的是,在电磁辐射发生时,要了解在何种条件下会发生载流子的传播共振条件。在本手稿中,我们推导了一个p–n异质结的色散关系,并将该方法应用于GaAs p–n结,这是光电器件的重要材料。考虑具有相等宽度的对称掺杂的p型和n型区域,研究了某些参数(例如掺杂和电压偏置)对p–n异质结色散曲线的影响。通过观察载体的不同有效质量和迁移率,我们能够获得对p和n区域产生相同介电功能的条件。我们的结果表明,p–n GaAs系统可以维持传播共振,并可以用作分层等离激元波导。可行的条件落在GaAs的横向光子声共振与二极管波导的传统截止频率之间的频率范围内。此外,我们的结果表明,当激发稍高于声子共振频率时,等离激元传播达到了低损耗特性。我们还表明,p-和n-界面之间耗尽区的存在或不存在使某些等离激元模传播,而另一些迅速衰减,这表明设计选择性滤波器的可能性。

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