1965
DOI: 10.1051/jphys:019650026011063900
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Selection rules for second order infrared and raman processes. I. Caesium chloride structure and interpretation of the second order Raman spectra of CsBr and Csi

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Cited by 14 publications
(2 citation statements)
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“…The caesium chloride structure also has a two-atom basis and thus three optical-phonon branches. However, the zone-center optical phonons here transform according to T 1u+ [40], i.e., like a spatial vector, which is plausible since the distortions generate an electric dipole moment of each unit cell. We denote the displacement vector by p = (p x , p y , p z ), which serves as the distortional order parameter.…”
Section: Distortion Modesmentioning
confidence: 99%
“…The caesium chloride structure also has a two-atom basis and thus three optical-phonon branches. However, the zone-center optical phonons here transform according to T 1u+ [40], i.e., like a spatial vector, which is plausible since the distortions generate an electric dipole moment of each unit cell. We denote the displacement vector by p = (p x , p y , p z ), which serves as the distortional order parameter.…”
Section: Distortion Modesmentioning
confidence: 99%
“…2. Experimental data are available for momentum-resolved phonon band structures of CsI 57 and NaI. 55,56 These are compared with theoretical predictions in Ref.…”
Section: Resultsmentioning
confidence: 99%