Abstract
Janus transition metal dichalcogenides (TMDs) lose the horizontal mirror symmetry of ordinary TMDs, leading to the emergence of additional features, such as native piezoelectricity, Rashba effect, and enhanced catalytic activity. While Raman spectroscopy is an essential nondestructive, phase- and composition-sensitive tool to monitor the synthesis of materials, a comprehensive study of the Raman spectrum of Janus monolayers is still missing. Here, we discuss the Raman spectra of WSSe and MoSSe measured at room and cryogenic temperatures, near and off resonance. By combining polarization-resolved Raman data with calculations of the phonon dispersion and using symmetry considerations, we identify the four first-order Raman modes and higher-order two-phonon modes. Moreover, we observe defect-activated phonon processes, which provide a route toward a quantitative assessment of the defect concentration and, thus, the crystal quality of the materials. Our work establishes a solid background for future research on material synthesis, study, and application of Janus TMD monolayers.
Original language | English |
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Article number | 035414 |
Journal | Physical Review B |
Volume | 103 |
Issue number | 3 |
DOIs | |
Publication status | Published - 15 Jan 2021 |
Externally published | Yes |
Bibliographical note
Publisher Copyright:© 2021 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.
Funding
We thank Moritz Meyer for technical assistance. S.T. acknowledges support from NSF DMR-1955889, NSF CMMI-1933214, NSF DMR-1552220, and DOE-SC0020653. K.M. and J.J.F. acknowledge support from the European Union Horizon 2020 research and innovation programme under Grant Agreement No. 820423 (S2QUIP) and the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy - MCQST (EXC-2111) and e-Conversion (EXC-2089). M.M.P. acknowledges TUM International Graduate School of Science and Engineering (IGSSE). M.K. acknowledges support from the International Max Planck Research School for Quantum Science and Technology (IMPRS-QST). M.B. acknowledges support from the Alexander von Humboldt Foundation. K.M. acknowledges support from the Bayerische Akademie der Wissenschaften. A.R.B.-M. acknowledges support from DGTIC-UNAM Supercomputing Center under Project LANCAD-UNAM-DGTIC-359.
Funders | Funder number |
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National Science Foundation |