Excitonic Dynamics in Janus MoSSe and WSSe MonolayersClick to copy article linkArticle link copied!
- Ting ZhengTing ZhengSchool of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, ChinaDepartment of Physics and Astronomy, The University of Kansas, Lawrence, Kansas 66045, United StatesMore by Ting Zheng
- Yu-Chuan Lin*Yu-Chuan Lin*Email: [email protected]Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesDepartment of Materials Science and Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United StatesMore by Yu-Chuan Lin
- Yiling YuYiling YuCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Yiling Yu
- Pavel Valencia-AcunaPavel Valencia-AcunaDepartment of Physics and Astronomy, The University of Kansas, Lawrence, Kansas 66045, United StatesMore by Pavel Valencia-Acuna
- Alexander A. PuretzkyAlexander A. PuretzkyCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Alexander A. Puretzky
- Riccardo TorsiRiccardo TorsiDepartment of Materials Science and Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United StatesMore by Riccardo Torsi
- Chenze LiuChenze LiuDepartment of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by Chenze Liu
- Ilia N. IvanovIlia N. IvanovCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Ilia N. Ivanov
- Gerd DuscherGerd DuscherDepartment of Materials Science and Engineering, University of Tennessee, Knoxville, Tennessee 37996, United StatesMore by Gerd Duscher
- David B. GeoheganDavid B. GeoheganCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by David B. Geohegan
- Zhenhua Ni*Zhenhua Ni*Email: [email protected]School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, ChinaMore by Zhenhua Ni
- Kai XiaoKai XiaoCenter for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, United StatesMore by Kai Xiao
- Hui Zhao*Hui Zhao*Email: [email protected]Department of Physics and Astronomy, The University of Kansas, Lawrence, Kansas 66045, United StatesMore by Hui Zhao
Abstract
We report here details of steady-state and time-resolved spectroscopy of excitonic dynamics for Janus transition metal dichalcogenide monolayers, including MoSSe and WSSe, which were synthesized by low-energy implantation of Se into transition metal disulfides. Absorbance and photoluminescence spectroscopic measurements determined the room-temperature exciton resonances for MoSSe and WSSe monolayers. Transient absorption measurements revealed that the excitons in Janus structures form faster than those in pristine transition metal dichalcogenides by about 30% due to their enhanced electron–phonon interaction by the built-in dipole moment. By combining steady-state photoluminescence quantum yield and time-resolved transient absorption measurements, we find that the exciton radiative recombination lifetime in Janus structures is significantly longer than in their pristine samples, supporting the predicted spatial separation of the electron and hole wave functions due to the built-in dipole moment. These results provide fundamental insight in the optical properties of Janus transition metal dichalcogenides.
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