The tuning of para- and diamagnetic cavity photon excitations in a square array of quantum dots in a magnetic field

Vidar Gudmundsson, Vram Mughnetsyan, Hsi-Sheng Goan, Jeng-Da Chai, Nzar Rauf Abdullah, Chi-Shung Tang, Valeriu Moldoveanu, Andrei Manolescu
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Abstract

We employ a ``real-time'' excitation scheme to calculate the excitation spectra of a two-dimensional electron system in a square array of quantum dots placed in a circular cylindrical far-infrared photon cavity subjected to a perpendicular homogeneous external magnetic field. The Coulomb interaction of the electrons is handled via spin density functional theory and the para- and the diamagnetic parts of the electron-photon coupling are updated according to a configuration interaction method in each iteration of the density functional calculation. The results show that an excitation scheme built on using the symmetry of the lateral square superlattice of the dots and the cylindrical cavity produces both para- and diamagnetic resonance peaks with oscillator strengths that can be steered by the excitation pulse parameters. The excitation method breaks the conditions for the generalized Kohn theorem and allows for insight into the subband structure of the electron system and can be used both in and outside the linear response regime.
方形量子点阵列在磁场中的顺磁腔和二磁腔光子激发调谐
我们采用一种 "实时 "激发方案来计算一个二维电子系统的激发谱,该电子系统位于一个正方形的量子点阵列中,该量子点阵列位于一个圆形的圆柱远红外光子腔中,并受到垂直的均匀外磁场的作用。电子的库仑相互作用是通过自旋密度泛函理论处理的,电子-光子耦合的顺磁和双磁部分是在密度泛函计算的每次迭代中根据构型相互作用方法更新的。结果表明,利用点的横向方形超晶格和圆柱形腔体的对称性建立的激发方案可以产生顺磁和二磁共振峰,其振荡强度可以通过激发脉冲参数来控制。该激发方法打破了广义科恩定理的条件,允许深入了解电子系统的子带结构,并可在线性响应机制内外使用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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