Kavli Energy NanoScience Institute , Berkeley , California 94720 , United States.
Department of Applied Physics , Stanford University , Stanford , California 94305 , United States.
Nano Lett. 2018 Oct 10;18(10):6135-6143. doi: 10.1021/acs.nanolett.8b01793. Epub 2018 Sep 13.
Layered transition metal dichalcogenides exhibit the emergence of a direct bandgap at the monolayer limit along with pronounced excitonic effects. In these materials, interaction with phonons is the dominant mechanism that limits the exciton coherence lifetime. Exciton-phonon interaction also facilitates energy and momentum relaxation, and influences exciton diffusion under most experimental conditions. However, the fundamental changes in the exciton-phonon interaction are not well understood as the material undergoes the transition from a direct to an indirect bandgap semiconductor. Here, we address this question through optical spectroscopy and microscopic theory. In the experiment, we study room-temperature statistics of the exciton line width for a large number of mono- and bilayer WS samples. We observe a systematic increase in the room-temperature line width of the bilayer compared to the monolayer of 50 meV, corresponding to an additional scattering rate of ∼0.1 fs. We further address both phonon emission and absorption processes by examining the temperature dependence of the width of the exciton resonances. Using a theoretical approach based on many-body formalism, we are able to explain the experimental results and establish a microscopic framework for exciton-phonon interactions that can be applied to naturally occurring and artificially prepared multilayer structures.
层状过渡金属二卤化物在单层极限处表现出直接带隙的出现以及明显的激子效应。在这些材料中,与声子的相互作用是限制激子相干寿命的主要机制。激子-声子相互作用还促进了能量和动量的弛豫,并在大多数实验条件下影响激子扩散。然而,当材料从直接带隙半导体转变为间接带隙半导体时,激子-声子相互作用的基本变化还没有得到很好的理解。在这里,我们通过光学光谱和微观理论来解决这个问题。在实验中,我们研究了大量单层和双层 WS 样品在室温下激子线宽的统计特性。我们观察到双层在室温下的线宽比单层系统增加了 50 meV,对应于附加的散射率约为 0.1 fs。我们通过研究激子共振宽度随温度的变化进一步研究了声子发射和吸收过程。我们使用基于多体形式主义的理论方法来解释实验结果,并建立了适用于自然发生和人工制备的多层结构的激子-声子相互作用的微观框架。