Please use this identifier to cite or link to this item: https://libjncir.jncasr.ac.in/xmlui/handle/10572/2348
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dc.contributor.authorLate, Dattatray J.
dc.contributor.authorShirodkar, Sharmila N.
dc.contributor.authorWaghmare, Umesh V.
dc.contributor.authorDravid, Vinayak P.
dc.contributor.authorRao, C. N. R.
dc.date.accessioned2017-02-21T06:56:21Z-
dc.date.available2017-02-21T06:56:21Z-
dc.date.issued2014
dc.identifier.citationLate, DJ; Shirodkar, SN; Waghmare, UV; Dravid, VP; Rao, CNR, Thermal Expansion, Anharmonicity and Temperature-Dependent Raman Spectra of Single- and Few-Layer MoSe2 and WSe2. Chemphyschem 2014, 15 (8) 1592-1598, http://dx.doi.org/10.1002/cphc.201400020en_US
dc.identifier.citationChemphyschemen_US
dc.identifier.citation15en_US
dc.identifier.citation8en_US
dc.identifier.issn1439-4235
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/2348-
dc.descriptionRestricted Accessen_US
dc.description.abstractWe report the temperature-dependent Raman spectra of single-and few-layer MoSe2 and WSe2 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(2u)(2) 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 MoS2 and of the G band of graphene. The temperature coefficients of the two modes in single-layer MoSe2 are larger than those of the same modes in single-layer WSe2. We have estimated thermal expansion coefficients and temperature dependence of the vibrational frequencies of MoS2 and MoSe2 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 MoS2 and MoSe2 arises essentially from the difference in their strainphonon coupling.en_US
dc.description.uri1439-7641en_US
dc.description.urihttp://dx.doi.org/10.1002/cphc.201400020en_US
dc.language.isoEnglishen_US
dc.publisherWiley-V C H Verlag Gmbhen_US
dc.rights@Wiley-V C H Verlag Gmbh, 2014en_US
dc.subjectPhysical Chemistryen_US
dc.subjectAtomic, Molecular & Chemical Physicsen_US
dc.subjectField-Effect Transistorsen_US
dc.subjectElectric-Fielden_US
dc.subjectSolar-Cellsen_US
dc.subjectGrapheneen_US
dc.subjectWs2en_US
dc.subjectFilmsen_US
dc.subjectGasen_US
dc.subjectSemiconductoren_US
dc.subjectElectronicsen_US
dc.subjectCrystalsen_US
dc.titleThermal Expansion, Anharmonicity and Temperature-Dependent Raman Spectra of Single- and Few-Layer MoSe2 and WSe2en_US
dc.typeArticleen_US
Appears in Collections:Research Articles (Umesh V. Waghmare)
Research Papers (Prof. C.N.R. Rao)

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