1984
DOI: 10.1143/jpsj.53.811
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Dispersive Raman Mode of Layered Compound 2H-MoS2 under the Resonant Condition

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Cited by 102 publications
(120 citation statements)
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“…The distinctive identity of the ∼377 cm −1 peak is further confirmed by its presence in pristine 1L-MoS 2 , where it manifests itself as a weak shoulder located at the low-frequency side of the E peak. The existence of a similar shoulder has been previously reported for bulk MoS 2 , and it has been assigned to Raman-inactive TO phonons with E 2 1u symmetry [33], arising from an atomic displacement pattern similar to that of E 1 2g . This assignment is questionable, as reflectivity measurements show this peak at the higher frequency side of the E peak [34].…”
Section: Resultssupporting
confidence: 80%
“…The distinctive identity of the ∼377 cm −1 peak is further confirmed by its presence in pristine 1L-MoS 2 , where it manifests itself as a weak shoulder located at the low-frequency side of the E peak. The existence of a similar shoulder has been previously reported for bulk MoS 2 , and it has been assigned to Raman-inactive TO phonons with E 2 1u symmetry [33], arising from an atomic displacement pattern similar to that of E 1 2g . This assignment is questionable, as reflectivity measurements show this peak at the higher frequency side of the E peak [34].…”
Section: Resultssupporting
confidence: 80%
“…The resonance Raman spectra show that multiple modes are shifted from the first-order Raman frequencies, which suggests that the electronic transitions are strongly coupled with phonon modes. There are several reports of this resonant Raman scattering phenomenon in MoS2 [78,79,86,91,93,[98][99][100]. All of these studies are in general agreement on the attribution of the peaks observed in the resonant Raman scattering spectrum, which suggests coupling between vibrational modes and longitudinal acoustic phonon modes.…”
Section: Resonant Raman Scatteringsupporting
confidence: 71%
“…The mode at ∼420 cm −1 is highly dispersive and explained by Sekine et al as a second-order Raman process, where a polariton created by the incident laser in a photon-like branch will first be scattered by emitting a longitudinal dispersive quasiacoustic (QA) phonon along Γ-A, and then scattered by emitting a E 2 1u phonon (which is dispersionless along Γ-A) into the exciton-like final state. 98 Here, Γ-A is perpendicular to the 2D Brillouin plane. The QA phonon at the Γ point is B (Γ-A) based on the excitonpolariton dispersion.…”
Section: Resonant Raman Scattering In Tmdsmentioning
confidence: 99%