Berry curvature and shift vector effects at high-order wave mixing in biased bilayer graphene

H. K. Avetissian, H. H. Matevosyan, G. F. Mkrtchian
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Abstract

In this work, we present a microscopic quantum theory that elucidates the nonlinear-nonperturbative optical response of biased bilayer graphene subjected to a bichromatic strong laser fields. This response is analyzed using a four-band Hamiltonian derived from ab-initio calculations. For the laser-stimulated dynamics, we employ structure gauge-invariant evolutionary equations to accurately describe the evolution of the single-particle density matrix across the entire Brillouin zone. The resonant generation of electron-hole pairs by the high-frequency component of the field, combined with the induction of high-order harmonic generation (HHG) and high-order wave mixing (HWM) by the strong low-frequency field component, leads to significant alterations in the HWM and HHG spectra. These changes are driven by the effects of Berry curvature and the shift vector, which modify the relative contributions of interband and intraband channels, thereby fundamentally reshaping the radiation spectra at high-order frequency multiplication.
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偏压双层石墨烯高阶波混合时的贝里曲率和位移矢量效应
在这项研究中,我们提出了一种微观量子理论,阐明了偏压双层石墨烯在双色强激光场作用下的非线性非微扰光学响应。这种响应是通过非线性计算得到的四带哈密顿来分析的。对于激光刺激的动力学,我们采用了结构规整不变的演化方程来精确描述整个布里渊区的单粒子密度矩阵的演化。高频场分量共振产生的电子-空穴对,加上强低频场分量诱导产生的高阶谐波(HHG)和高阶混波(HWM),导致 HWM 和 HHG 光谱发生显著变化。这些变化是由贝里曲率和位移矢量的影响驱动的,它们改变了带间和带内信道的相对贡献,从而从根本上重塑了高阶频率倍增时的辐射光谱。
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