1985
DOI: 10.1016/0022-3697(85)90103-9
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Raman spectra of IVB and VIB transition metal disulfides using laser energies near the absorption edges

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Cited by 137 publications
(137 citation statements)
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“…The asymmetric 2LA(M) peak is associated with second-order zoneedge phonon (LA(M)) and a first order optical phonon peak (A 2u ). [55][56][57][58] These results along with electron microscopy results suggests that the structure is relatively undistorted MoS 2 . [59][60] Further, X-ray diffraction analysis (XRD) of MoS 2 -raw and MoS 2 -SA in Fig.…”
Section: Resultsmentioning
confidence: 73%
“…The asymmetric 2LA(M) peak is associated with second-order zoneedge phonon (LA(M)) and a first order optical phonon peak (A 2u ). [55][56][57][58] These results along with electron microscopy results suggests that the structure is relatively undistorted MoS 2 . [59][60] Further, X-ray diffraction analysis (XRD) of MoS 2 -raw and MoS 2 -SA in Fig.…”
Section: Resultsmentioning
confidence: 73%
“…Figures 20(c) and (d) show the lateral view of the The experimental data has been collected from several publications, red squares [43], red and blue circles [10], green circles [11] and green triangles [110].…”
Section: Bethe-salpeter Equation Formalismmentioning
confidence: 99%
“…The E1g mode and E2g 2 mode usually cannot be detected by conventional Raman Scattering measurements. The weak intensity of the E1g mode is due to the laser polarization chosen and random crystal direction of different MoS2 samples [86]. For example, the E1g mode is forbidden for s-polarized laser light incident on the MoS2 crystal surface (the E field is perpendicular to the c-axis of MoS2) [85].…”
Section: Lattice Dynamic: Raman Scattering and Ir Absorptionmentioning
confidence: 99%