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Theory of excitonic high-order sideband generation in semiconductors under a strong terahertz field

机译:强太赫兹场下半导体中激子高阶边带产生的理论

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We present the theory of excitonic high-order sideband generation (HSG) in semiconductors by an intense terahertz (THz) field. When the Coulomb interaction is neglected, we give an analytical solution to the HSG with the help of Floquet theory. Besides, the HSG is also studied by the quantum trajectory theory (saddle-point method) by which the HSG is explained by the interference of different quantum trajectories of excitons when accelerating in the external THz field. Both the exact analytic solution and the saddle-point method obtain consistent results: the spectrum of sidebands has an extended plateau where all the sidebands have almost the same intensity, which is similar to the high-order harmonic generation in atomic system. Moreover the HSG provides more flexibility in studying the quantum trajectory theory. When Coulomb interaction is considered, we find considerable Coulomb enhancement of HSG, which is absent in atomic system. The mechanism is discussed based on numerical calculations.
机译:我们通过强太赫兹(THz)场介绍了半导体中激子高阶边带生成(HSG)的理论。当忽略库仑相互作用时,我们借助Floquet理论为HSG提供了解析解决方案。此外,还通过量子轨迹理论(马鞍点法)研究了HSG,通过在外部太赫兹场中加速时激子的不同量子轨迹的干扰来解释HSG。精确的解析解和鞍点法都获得了一致的结果:边带的频谱具有扩展的平台,其中所有边带的强度几乎相同,这类似于原子系统中高次谐波的产生。此外,HSG在研究量子轨迹理论方面提供了更大的灵活性。当考虑库仑相互作用时,我们发现HSG有相当大的库仑增强,这在原子系统中是不存在的。基于数值计算讨论了该机制。

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