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Theory of optical excitations in dipole-coupled hybrid molecule-semiconductor layers: Coupling of a molecular resonance to semiconductor continuum states

机译:偶极子耦合杂化分子 - 半导体层中的光学激发理论:分子共振与半导体连续体状态的耦合

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摘要

We theoretically investigate the optical absorption of a hybrid system consisting of an organic molecular lm on top of a semiconductor substrate. The electronic states of the isolated spatially separated constituents couple due to the Coulomb interaction of the optically induced charge carriers across the lm-substrate interface. Focussing on the coupling of optical active molecular transitions to semiconductor continuum states, we nd that the non-radiative dipole-dipole energy transfer causes the formation of coupled excitations, eectively reducing the excitation energy of the optical resonance in the molecular lm and inducing a broadening of the associated absorption peak. In the framework of the Heisenberg equation of motion technique we derive the Bloch equations for these hybrid systems. The input parameters for our model system of ladder-type quarterphenyl (L4P) molecules on the ZnO(1010) surface are taken from density functional theory calculations.
机译:我们从理论上研究了由有机分子lm组成的混合系统在半导体衬底顶部的光吸收。分离的空间上分离的成分的电子状态由于跨lm-衬底界面的光感应电荷载流子的库仑相互作用而耦合。着眼于光学活性分子跃迁与半导体连续态的耦合,我们发现非辐射偶极-偶极能量转移引起耦合激发的形成,有效地降低了分子lm中光学共振的激发能并引起了变宽。相关吸收峰的最大值。在海森堡运动技术方程的框架中,我们导出了这些混合系统的布洛赫方程。我们的ZnO(1010)表面上的梯型四苯基(L4P)分子模型系统的输入参数来自密度泛函理论计算。

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