1968
DOI: 10.1103/physrev.171.931
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Raman Effect in Wurtzite- and Zinc-Blende-Type ZnS Single Crystals

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Cited by 230 publications
(128 citation statements)
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“…However, in the present study, we cannot assign this peak to the TO mode of cubic ZnS because the zone center and zone boundary TO phonon for bulk cubic ZnS are reported to appear at 276 and 303 cm -1 , respectively [42,43]. Brafman and Mitra [44] reported the TO and LO zone center phonons of cubic ZnS crystals to be at 276 and 351 cm -1 respectively, for the Raman spectra of bulk cubic phases of ZnS. According to Smith [45], the coupling between longitudinal phonons and charge density fluctuations (plasmons) in polar semi-conducting systems results in two different LO phonon-plasmon coupled modes (LOPC modes), namely the L + and L -modes.…”
Section: Raman Spectroscopymentioning
confidence: 91%
“…However, in the present study, we cannot assign this peak to the TO mode of cubic ZnS because the zone center and zone boundary TO phonon for bulk cubic ZnS are reported to appear at 276 and 303 cm -1 , respectively [42,43]. Brafman and Mitra [44] reported the TO and LO zone center phonons of cubic ZnS crystals to be at 276 and 351 cm -1 respectively, for the Raman spectra of bulk cubic phases of ZnS. According to Smith [45], the coupling between longitudinal phonons and charge density fluctuations (plasmons) in polar semi-conducting systems results in two different LO phonon-plasmon coupled modes (LOPC modes), namely the L + and L -modes.…”
Section: Raman Spectroscopymentioning
confidence: 91%
“…B 1 modes are inactive in both the spectra. 31,32 The A 1 and E 1 symmetry can split into two components: transverse optic (TO) and longitudinal optic (LO), and both of them are highly isotropic, A 1 (TO) = E 1 (TO) and A 1 (LO) = E 1 (LO), which is a characteristic feature of the wurtzite ZnS. 31,33 Fig.…”
Section: B Micro Raman Spectral Analysismentioning
confidence: 99%
“…The value of /~cds calculated using equations (3.1) of Hewat (1972) is 1.01 A 2. The elastic constants used were those of Berlincourt, Jaffe & Shiozawa (1963) and the average value of Wo 2 (where too is the zone-centre frequency determined by Raman scattering) was calculated using the data of Tell, Damen & Porto (1966) and Brafman & Mitra (1968). Table 4 show that the parameter values for S are more difficult to determine than those for Cd.…”
Section: Observedmentioning
confidence: 99%