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随机散射理论在激发诱导退相中的应用:时变非线性相干激子线宽。

Stochastic scattering theory for excitation-induced dephasing: Time-dependent nonlinear coherent exciton lineshapes.

机构信息

Department of Physics and Center for Functional Materials, Wake Forest University, 1834 Wake Forest Road, Winston-Salem, North Carolina 27109, USA.

Department of Chemistry, University of Houston, Houston, Texas 77204, USA.

出版信息

J Chem Phys. 2020 Oct 28;153(16):164706. doi: 10.1063/5.0026351.

Abstract

We develop a stochastic theory that treats time-dependent exciton-exciton s-wave scattering and that accounts for dynamic Coulomb screening, which we describe within a mean-field limit. With this theory, we model excitation-induced dephasing effects on time-resolved two-dimensional coherent optical lineshapes and we identify a number of features that can be attributed to the many-body dynamics occurring in the background of the exciton, including dynamic line narrowing, mixing of real and imaginary spectral components, and multi-quantum states. We test the model by means of multidimensional coherent spectroscopy on a two-dimensional metal-halide semiconductor that hosts tightly bound excitons and biexcitons that feature strong polaronic character. We find that the exciton nonlinear coherent lineshape reflects many-body correlations that give rise to excitation-induced dephasing. Furthermore, we observe that the exciton lineshape evolves with the population time over time windows in which the population itself is static in a manner that reveals the evolution of the multi-exciton many-body couplings. Specifically, the dephasing dynamics slow down with time, at a rate that is governed by the strength of exciton many-body interactions and on the dynamic Coulomb screening potential. The real part of the coherent optical lineshape displays strong dispersive character at zero time, which transforms to an absorptive lineshape on the dissipation timescale of excitation-induced dephasing effects, while the imaginary part displays converse behavior. Our microscopic theoretical approach is sufficiently flexible to allow for a wide exploration of how system-bath dynamics contribute to linear and non-linear time-resolved spectral behavior.

摘要

我们提出了一种处理时变激子-激子 s 波散射的随机理论,并考虑了动态库仑屏蔽,我们在平均场极限内对其进行了描述。利用这一理论,我们对激发诱导的退相效应对时间分辨二维相干光学线谱进行建模,并确定了一些可以归因于激子背景中多体动力学的特征,包括动态线宽变窄、实部和虚部谱分量的混合以及多量子态。我们通过二维金属卤化物半导体的多维相干光谱学对该模型进行了测试,该半导体中含有紧密束缚的激子和具有强极化子特性的双激子。我们发现,激子非线性相干线谱反映了多体相关性,这些相关性导致了激发诱导的退相。此外,我们观察到激子线谱随时间演化,在种群本身在静态的时间窗口中演化,这揭示了多激子多体耦合的演化。具体来说,退相动力学随时间减缓,速率由激子多体相互作用的强度和动态库仑屏蔽势决定。相干光学线谱的实部在零时显示出很强的色散特征,在激发诱导退相效应的耗散时间尺度上转变为吸收线谱,而虚部则显示出相反的行为。我们的微观理论方法足够灵活,可以广泛探索系统-浴动力学如何影响线性和非线性时间分辨光谱行为。

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