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Role of quantum coherence in shaping the line shape of an exciton interacting with a spatially and temporally correlated bath

机译:量子相干在塑造与时空相关的浴相互作用的激子的线形中的作用

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摘要

Kubo’s fluctuation theory of line shape forms the backbone of our understanding of optical and vibrational line shapes, through such concepts as static heterogeneity and motional narrowing. However, the theory does not properly address the effects of quantum coherences on optical line shape, especially in extended systems where a large number of eigenstates are present. In this work, we study the line shape of an exciton in a one-dimensional lattice consisting of regularly placed and equally separated optical two level systems. We consider both linear array and cyclic ring systems of different sizes. Detailed analytical calculations of line shape have been carried out by using Kubo’s stochastic Liouville equation (SLE). We make use of the observation that in the site representation, the Hamiltonian of our system with constant off-diagonal coupling J is a tridiagonal Toeplitz matrix (TDTM) whose eigenvalues and eigenfunctions are known analytically. This identification is particularly useful for long chains where the eigenvalues of TDTM help understanding crossover between static and fast modulation limits. We summarize the new results as follows. (i) In the slow modulation limit when the bath correlation time is large, the effects of spatial correlation are not negligible. Here the line shape is broadened and the number of peaks increases beyond the ones obtained from TDTM (constant off-diagonal coupling element J and no fluctuation). (ii) However, in the fast modulation limit when the bath correlation time is small, the spatial correlation is less important. In this limit, the line shape shows motional narrowing with peaks at the values predicted by TDTM (constant J and no fluctuation). (iii) Importantly, we find that the line shape can capture that quantum coherence affects in the two limits differently. (iv) In addition to linear chains of two level systems, we also consider a cyclic tetramer. The cyclic polymers can be designed for experimental verification. (v) We also build a connection between line shape and population transfer dynamics. In the fast modulation limit, both the line shape and the population relaxation, for both correlated and uncorrelated bath, show similar behavior. However, in slow modulation limit, they show profoundly different behavior. (vi) This study explains the unique role of the rate of fluctuation (inverse of the bath correlation time) in the sustenance and propagation of coherence. We also examine the effects of off-diagonal fluctuation in spectral line shape. Finally, we use Tanimura-Kubo formalism to derive a set of coupled equations to include temperature effects (partly neglected in the SLE employed here) and effects of vibrational mode in energy transfer dynamics.
机译:久保的线形波动理论通过诸如静态异质性和运动变窄之类的概念,构成了我们对光学和振动线形理解的基础。但是,该理论不能正确解决量子相干对光线形状的影响,尤其是在存在大量本征态的扩展系统中。在这项工作中,我们研究一维激子在由规则放置和均等分离的光学两级系统组成的一维晶格中的线形。我们考虑了不同大小的线性阵列和环状环系统。通过使用Kubo的随机Liouville方程(SLE)进行了详细的线形分析计算。我们利用以下观察结果:在站点表示中,具有恒定斜对角耦合J的系统的哈密顿量是一个三对角Toeplitz矩阵(TDTM),其特征值和特征函数在解析上是已知的。此标识对于长链特别有用,在长链中,TDTM的特征值有助于理解静态和快速调制限制之间的交叉。我们将新结果总结如下。 (i)在浴相关时间长的慢调制极限中,空间相关的影响不可忽略。在此,线形变宽,并且峰的数量增加,超过了从TDTM获得的峰(恒定的非对角线耦合元素J,无波动)。 (ii)但是,在浴相关时间短的快速调制极限中,空间相关性不太重要。在此限制下,线形显示运动变窄,在TDTM预测的值处出现峰值(恒定J且无波动)。 (iii)重要的是,我们发现线形可以捕获量子相干性在两个极限中的不同影响。 (iv)除了两级系统的线性链,我们还考虑了环状四聚体。环状聚合物可以设计用于实验验证。 (v)我们还在线形和人口转移动力学之间建立联系。在快速调制极限中,相关浴和不相关浴的线形和总体弛豫都表现出相似的行为。但是,在慢速调制极限下,它们表现出截然不同的行为。 (vi)这项研究解释了波动率(浴相关时间的倒数)在相干的维持和传播中的独特作用。我们还检查了谱线形状中非对角线波动的影响。最后,我们使用Tanimura-Kubo形式主义来导出一组耦合方程,以包括温度效应(在此采用的SLE中被部分忽略)和振动模式在能量传递动力学中的效应。

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