2001
DOI: 10.1002/1521-3951(200101)223:1<331::aid-pssb331>3.0.co;2-e
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Effect of Pressure on the Anomalous Raman Spectrum of CuBr

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Cited by 6 publications
(2 citation statements)
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“…The Fermi resonance is a rare phenomenon in solids that has been observed in copper halides, molecules and defect modes. [76][77][78][79] In SnSb2Te4, the sum of the frequencies of the Ag 1 and Eg 1 at  almost coincides in frequency with the Eg 2 mode at 2 GPa; i.e. the pressure range close to the onset of the softening of this mode in SnSb2Te4 (Figure 6).…”
Section: Raman Scattering Measurements Under Pressurementioning
confidence: 99%
“…The Fermi resonance is a rare phenomenon in solids that has been observed in copper halides, molecules and defect modes. [76][77][78][79] In SnSb2Te4, the sum of the frequencies of the Ag 1 and Eg 1 at  almost coincides in frequency with the Eg 2 mode at 2 GPa; i.e. the pressure range close to the onset of the softening of this mode in SnSb2Te4 (Figure 6).…”
Section: Raman Scattering Measurements Under Pressurementioning
confidence: 99%
“…In recent low-temperature Raman studies of Si, Ge, CuCl, CuBr and GaP [56][57][58][59] it was demonstrated that pressure-induced changes in the TO and/or LO line widths can be well explained by variations in the rate at which zone-centre optical phonons decay into zero-wavevector two-phonon combinations due to third-order anharmonic coupling. The anharmonic line broadening is determined by the imaginary part (ω) of the phonon selfenergy, which is proportional to the q = 0 two-phonon density of states weighted by thermal population factors [55].…”
Section: Raman Line Widthsmentioning
confidence: 99%