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Effects of the Structure and Temperature on the Nature of Excitons in the Mo0.6W0.4S2 Alloy
Author(s) -
Deepika Poonia,
Nisha Singh,
Jeff J. P. M. Schulpen,
Marco van der Laan,
Sourav Maiti,
Michele Failla,
Sachin Kinge,
Ageeth A. Bol,
Peter Schall,
Laurens D. A. Siebbeles
Publication year - 2022
Publication title -
the journal of physical chemistry c
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.401
H-Index - 289
eISSN - 1932-7455
pISSN - 1932-7447
DOI - 10.1021/acs.jpcc.1c09806
Subject(s) - exciton , time dependent density functional theory , alloy , absorption spectroscopy , materials science , spectral line , spectroscopy , phonon , density functional theory , absorption (acoustics) , molecular physics , atomic physics , condensed matter physics , chemistry , computational chemistry , physics , optics , quantum mechanics , astronomy , composite material
We studied the nature of excitons in the transition metal dichalcogenide alloy Mo 0.6 W 0.4 S 2 compared to pure MoS 2 and WS 2 grown by atomic layer deposition (ALD). For this, optical absorption/transmission spectroscopy and time-dependent density functional theory (TDDFT) were used. The effects of temperature on A and B exciton peak energies and line widths in optical transmission spectra were compared between the alloy and pure MoS 2 and WS 2 . On increasing the temperature from 25 to 293 K, the energy of the A and B exciton peaks decreases, while their line width increases due to exciton-phonon interactions. The exciton-phonon interactions in the alloy are closer to those for MoS 2 than those for WS 2 . This suggests that exciton wave functions in the alloy have a larger amplitude on Mo atoms than that on W atoms. The experimental absorption spectra could be reproduced by TDDFT calculations. Interestingly, for the alloy, the Mo and W atoms had to be distributed over all layers. Conversely, we could not reproduce the experimental alloy spectrum by calculations on a structure with alternating layers, in which every other layer contains only Mo atoms and the layers in between also contain W atoms. For the latter atomic arrangement, the TDDFT calculations yielded an additional optical absorption peak that could be due to excitons with some charge transfer character. From these results, we conclude that ALD yields an alloy in which Mo and W atoms are distributed uniformly among all layers.

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