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Thermal Expansion, Anharmonicity and Temperature‐Dependent Raman Spectra of Single‐ and Few‐Layer MoSe 2 and WSe 2
Author(s) -
Late Dattatray J.,
Shirodkar Sharmila N.,
Waghmare Umesh V.,
Dravid Vinayak P.,
Rao C. N. R.
Publication year - 2014
Publication title -
chemphyschem
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.016
H-Index - 140
eISSN - 1439-7641
pISSN - 1439-4235
DOI - 10.1002/cphc.201400020
Subject(s) - anharmonicity , raman spectroscopy , thermal expansion , phonon , atmospheric temperature range , condensed matter physics , materials science , graphene , molecular physics , spectral line , chemistry , analytical chemistry (journal) , optics , nanotechnology , physics , thermodynamics , chromatography , astronomy , metallurgy
We report the temperature‐dependent Raman spectra of single‐ and few‐layer MoSe 2 and WSe 2 in the range 77–700 K. We observed linear variation in the peak positions and widths of the bands arising from contributions of anharmonicity and thermal expansion. After characterization using atomic force microscopy and high‐resolution transmission electron microscopy, the temperature coefficients of the Raman modes were determined. Interestingly, the temperature coefficient of the A 2 2u mode is larger than that of the A 1g mode, the latter being much smaller than the corresponding temperature coefficients of the same mode in single‐layer MoS 2 and of the G band of graphene. The temperature coefficients of the two modes in single‐layer MoSe 2 are larger than those of the same modes in single‐layer WSe 2 . We have estimated thermal expansion coefficients and temperature dependence of the vibrational frequencies of MoS 2 and MoSe 2 within a quasi‐harmonic approximation, with inputs from first‐principles calculations based on density functional theory. We show that the contrasting temperature dependence of the Raman‐active mode A 1g in MoS 2 and MoSe 2 arises essentially from the difference in their strain–phonon coupling.