1974
DOI: 10.1016/s0022-3697(74)80137-x
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Shell model lattice dynamics of transition metal oxides

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Cited by 27 publications
(9 citation statements)
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“…Indeed, a weak multiphonon structure close to 400 cm −1 has been calculated by Upadhyaya and Singh. 52 However, much stronger peaks in the combined density of states are calculated to appear close to 435, 500, and 535 cm −1 , which could not be identified unambiguously. In addition, it has to be stated that the temperature dependence of the observed structures ͓inset ͑b͒ of Fig.…”
Section: Resultsmentioning
confidence: 92%
“…Indeed, a weak multiphonon structure close to 400 cm −1 has been calculated by Upadhyaya and Singh. 52 However, much stronger peaks in the combined density of states are calculated to appear close to 435, 500, and 535 cm −1 , which could not be identified unambiguously. In addition, it has to be stated that the temperature dependence of the observed structures ͓inset ͑b͒ of Fig.…”
Section: Resultsmentioning
confidence: 92%
“…[18] or 500 cm −1 in Ref. [19]. The highest frequency band at 1050 cm −1 has complex origin: it envelops two bands related to the TO + LO (a band wing at 950 cm −1 ) and 2LO modes.…”
Section: Resultsmentioning
confidence: 92%
“…The last four parameters are determined by the knowledge of electrical polarizability (α 1 , α 2 ) and the zone center optical vibration frequencies (ω L , ω T ) given by eqs. (8), (9), (11), and…”
Section: Both Ions Polarizable Model (Bipm)mentioning
confidence: 99%
“…The strange features in the nature and physical properties of TMO in the paramagnetic phase (NaCl Structure) has given an increased interest in the study of their lattice dynamics. The lattice dynamics of MnO, CoO and NiO has been studied in detail by many experimental [7][8][9][10] and theoretical workers [11][12][13][14] with great success. While such studies for FeO (wustite) 15) has met only with moderate success.…”
Section: §1 Introductionmentioning
confidence: 99%