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All-optical coherent control of electrical currents in centrosymmetric semiconductors

机译:中心对称半导体中电流的全光相干控制

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The absorption of phase-related near-infrared fundamental (ω,0.7 eV ≤ hω ≤ 0.9 eV) and second harmonic (2ω ) pulses of 150 fs duration results in ballistic electrical currents in clean bulk germanium and silicon at room temperature. The ultrafast charge motion is directly monitored via a time-resolved analysis of the emitted bursts of terahertz radiation. The current generation process relies on a third-order optical nonlinearity with a current injection efficiency only slightly reduced compared to the established current injection in direct-gap semiconductors such as GaAs. In the present case, current injection takes place across the direct band gap of germanium, whereas it involves indirect optical transitions in silicon. The vector direction of the current is defined by the polarization of the two-color pump field and the relative phase △φ=2φ_ω-φ_2ω Microscopically, current injection can be understood as arising from the quantum interference of one- and two-photon absorption processes. In the case of silicon, these indirect optical transitions may involve different types of phonons and can occur via numerous pathways. We therefore propose a model based on third-order perturbation theory which qualitatively explains why a current injection can occur across an indirect band gap.
机译:相位相关的近红外基波(ω,0.7 eV≤hω≤0.9 eV)和150 fs持续时间的二次谐波(2ω)脉冲的吸收会在室温下在干净的大块锗和硅中产生弹道电流。通过对太赫兹辐射发射脉冲的时间分辨分析,可以直接监视超快电荷运动。电流产生过程依赖于三次光学非线性,其电流注入效率与直接间隙半导体(如GaAs)中已建立的电流注入相比仅略有降低。在当前情况下,电流注入发生在锗的直接带隙上,而它涉及硅中的间接光学跃迁。电流的矢量方向由双色泵浦场的极化和相对相位△φ=2φ_ω-φ_2ω定义。从微观上讲,电流注入可以理解为是由一光子吸收和两光子吸收过程的量子干涉引起的。在硅的情况下,这些间接的光学跃迁可能涉及不同类型的声子,并可能通过多种途径发生。因此,我们提出了一个基于三阶微扰理论的模型,该模型定性地解释了为什么电流注入会跨越间接带隙发生。

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