Xu Ce, Zhou Guoqing, Alexeev Evgeny M, Cadore Alisson R, Paradisanos Ioannis, Ott Anna K, Soavi Giancarlo, Tongay Sefaattin, Cerullo Giulio, Ferrari Andrea C, Prezhdo Oleg V, Loh Zhi-Heng
School of Chemistry, Chemical Engineering and Biotechnology, and School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371, Singapore.
Department of Physics and Astronomy, University of Southern California, Los Angeles, California 90089, United States.
ACS Nano. 2023 Sep 12;17(17):16682-16694. doi: 10.1021/acsnano.3c02917. Epub 2023 Aug 15.
Strain engineering is an attractive approach for tuning the local optoelectronic properties of transition metal dichalcogenides (TMDs). While strain has been shown to affect the nanosecond carrier recombination dynamics of TMDs, its influence on the sub-picosecond electronic relaxation dynamics is still unexplored. Here, we employ a combination of time-resolved photoemission electron microscopy (TR-PEEM) and nonadiabatic molecular dynamics (NAMD) to investigate the ultrafast dynamics of wrinkled multilayer (ML) MoS comprising 17 layers. Following 2.41 eV photoexcitation, electronic relaxation at the Γ valley occurs with a time constant of 97 ± 2 fs for wrinkled ML-MoS and 120 ± 2 fs for flat ML-MoS. NAMD shows that wrinkling permits larger amplitude motions of MoS layers, relaxes electron-phonon coupling selection rules, perturbs chemical bonding, and increases the electronic density of states. As a result, the nonadiabatic coupling grows and electronic relaxation becomes faster compared to flat ML-MoS. Our study suggests that the sub-picosecond electronic relaxation dynamics of TMDs is amenable to strain engineering and that applications which require long-lived hot carriers, such as hot-electron-driven light harvesting and photocatalysis, should employ wrinkle-free TMDs.
应变工程是一种用于调节过渡金属二硫属化物(TMDs)局部光电特性的有吸引力的方法。虽然应变已被证明会影响TMDs的纳秒级载流子复合动力学,但其对亚皮秒级电子弛豫动力学的影响仍未被探索。在这里,我们结合时间分辨光发射电子显微镜(TR-PEEM)和非绝热分子动力学(NAMD)来研究包含17层的褶皱多层(ML)MoS₂的超快动力学。在2.41 eV光激发后,对于褶皱ML-MoS₂,Γ谷处的电子弛豫时间常数为97±2 fs,而对于平整ML-MoS₂,该时间常数为120±2 fs。NAMD表明,褶皱允许MoS₂层有更大幅度的运动,放宽了电子-声子耦合选择规则,扰动了化学键,并增加了态密度。结果,与平整ML-MoS₂相比,非绝热耦合增强,电子弛豫变得更快。我们的研究表明,TMDs的亚皮秒级电子弛豫动力学适合应变工程,并且需要长寿命热载流子的应用,如热电子驱动的光捕获和光催化,应采用无褶皱的TMDs。