2007
DOI: 10.1134/s1054660x07060072
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Theoretical treatment of the second-order Raman scattering

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Cited by 4 publications
(3 citation statements)
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“…This is why the P 3 peak is present in UV Raman spectrum but not detectable via visible-light Raman experiments. 33 Prior theoretical studies of monolayers 31 find a Raman active normal mode for both crystals between 530 and 550 cm −1 . However, as shown in Figures 2a,b, the silicon substrate also shows an intense peak at 520 cm −1 which masks Raman features originating from the MPX 3 crystals.…”
Section: Resultsmentioning
confidence: 97%
See 1 more Smart Citation
“…This is why the P 3 peak is present in UV Raman spectrum but not detectable via visible-light Raman experiments. 33 Prior theoretical studies of monolayers 31 find a Raman active normal mode for both crystals between 530 and 550 cm −1 . However, as shown in Figures 2a,b, the silicon substrate also shows an intense peak at 520 cm −1 which masks Raman features originating from the MPX 3 crystals.…”
Section: Resultsmentioning
confidence: 97%
“…, the higher the incident photon energy, the higher the second-order scattering cross section. This is why the P 3 peak is present in UV Raman spectrum but not detectable via visible-light Raman experiments …”
Section: Resultsmentioning
confidence: 99%
“…More importantly, the damage appeared as a 'double-lung' pattern, which cannot be predicted by small-aperture laser-induced damage tests. We find that the 'double-lung' damage is mainly due to transverse stimulated Raman scattering (SRS) effect [12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%