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Transmission Line Theory of Collective Plasma Excitations in Periodic Two-Dimensional Electron Systems: Finite Plasmonic Crystals and Tamm States

机译:周期集体等离子体激发的传输线理论   二维电子系统:有限等离子体晶体和Tamm态

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摘要

We present a comprehensive theory of the one-dimensional plasmonic crystalformed in the grating gated two-dimensional electron gas (2DEG) insemiconductor heterostructures. To describe collective plasma excitations inthe 2DEG, we develop a generalized transmission line theoretical formalismconsistent with the plasma hydrodynamic model. We then apply this formalism toanalyze the plasmonic spectra of 2DEG systems with step-like periodic changesof electron density and/or gate screening. We show that in a periodicallymodulated 2DEG, a plasmonic crystal is formed and derive closed-form analyticalexpressions describing its energy band spectrum for both infinite and finitesize crystals. Our results demonstrate a non-monotonic dependence of theplasmonic band gap width on the electron density modulation. At so-calledtransparency points where the plasmon propagates through the periodic 2DEG in aresonant manner, the plasmonic band gaps vanish. In semi-infinite plasmoniccrystals, we demonstrate the formation of plasmonic Tamm states andanalytically derive their energy dispersion and spatial localization. Finally,we present detailed numerical analysis of the plasmonic band structure of afinite four-period plasmonic crystal terminated either by an Ohmic contact orby an infinite barrier on each side. We trace the evolution of the plasmonicband spectrum, including the Tamm states, with changing electron densitymodulation and analyze the boundary conditions necessary for formation of theTamm states. We also analyze interaction between the Tamm states formed at theopposite edges of the short length plasmonic crystal. The validity of ourtheoretical approach was confirmed in experimental studies of plasmoniccrystals in short modulated plasmonic cavities which demonstrated excellentquantitative agreement between theory and experiment.
机译:我们提出了在栅控二维电子气(2DEG)半导体异质结构中形成的一维等离子体激元的综合理论。为了描述2DEG中的集体等离子体激发,我们开发了与等离子体流体动力学模型一致的广义传输线理论形式。然后,我们采用这种形式主义来分析2DEG系统的等离激元光谱,并逐步改变电子密度和/或进行栅极筛选。我们表明,在周期性调制的2DEG中,形成了等离激元晶体,并得出描述其能带谱的无穷和有限尺寸晶体的闭式分析表达式。我们的结果证明等离激元带隙宽度对电子密度调制的非单调依赖性。在等离激元以共振方式通过周期性2DEG传播的所谓透明点处,等离激元带隙消失了。在半无限长的等离子体晶体中,我们证明了等离子体Tamm态的形成,并解析得出了它们的能量色散和空间局域性。最后,我们给出了由欧姆接触或两侧的无限势垒终止的无限四周期等离子体激元晶体的等离子体能带结构的详细数值分析。我们跟踪变化的电子密度调制,包括Tamm态等离子带谱的演变,并分析了形成Tamm态所必需的边界条件。我们还分析了在短长度等离激元晶体的相反边缘形成的Tamm态之间的相互作用。我们的理论方法的有效性在短调制等离子体腔中的等离子体晶体的实验研究中得到了证实,该实验证明了理论与实验之间的良好定量一致性。

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