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Dispersive Raman Mode of Layered Compound 2H-MoS<sub>2</sub> under the Resonant Condition
101
Citations
20
References
1984
Year
EngineeringLaser ScienceSpectroscopic PropertyRaman PeakOptical PropertiesResonant ConditionQuantum MaterialsA ExcitonPhotonicsPhysicsLaser SpectroscopyLayered MaterialB ExcitonTransition Metal ChalcogenidesNatural SciencesSpectroscopyApplied PhysicsCondensed Matter PhysicsPhononDispersive Raman Mode
A frequency shift of a Raman peak is observed in 2H-MoS 2 , when the exciting laser frequency ω i is tuned across the A and B excitonic levels. The frequency shift decreases as ω i increases. It can be explained as due to a resonant two-phonon Raman process of the successive emission of a dispersive longitudinal quasi-acoustic phonon and a dispersionless E 1u 2 phonon both along the c axis. The translational exciton masses along the c axis are estimated to be (1.3 ±0.2) m 0 for the 1 s state of the A exciton and (1.6 ±0.3) m 0 for the 1 s state of the B exciton. The observed Raman cross section is consistent with qualitative estimation in terms of this Raman process.
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