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Theoretical study of electron dynamics in graphene interacting with ultrafast and ultrastrong laser pulses

机译:石墨烯中电子动力学与超快超强激光脉冲相互作用的理论研究

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In this paper, we investigate the dynamics of electron system in graphene monolayer from the theoretical and numerical points of view. We have shown that graphene subjected to an ultrafast (near-single-oscillation pulse) and strong (on the order of interatomic field) pulse, exhibits fundamental behavior dramatically different from both insulators and metals. In such an ultrafast and ultrastrong field, the electron dynamics is coherent and is described by time-dependent Schrodinger equation. Electron transfer from Valence band to Conduction band is deeply irreversible which implies non-adiabaticity of the system in which the residual Conduction band population (after the pulse ends) is close to the maximum one. The residual Conduction band populations a function of wave vector is non-uniform with a few strongly localized spots near the Dirac points, at which the Conduction band is almost fully populated.
机译:本文从理论和数值的角度研究了石墨烯单层电子系统的动力学。我们已经证明,石墨烯受到超快(近单振荡脉冲)和强(按原子间场的阶数)脉冲的作用,表现出与绝缘体和金属截然不同的基本行为。在这样的超快速和超强场中,电子动力学是连贯的,并由与时间有关的薛定inger方程来描述。电子从价带到导带的转移是不可逆的,这意味着系统的绝热性(其中剩余的导带总数(在脉冲结束后)接近最大)。剩余的导带的波动函数是不均匀的,在Dirac点附近有一些强烈的局部斑点,在该点处导带几乎完全填充。

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