2005
DOI: 10.1002/crat.200410536
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Adiabatic bond charge model for lattice dynamics of ternary chalcopyrite semiconductors

Abstract: The adiabatic bond charge model of Rustagi and Weber is extended to study lattice dynamical properties of ternary chalcopyrite semiconductors AgGaS 2 , AgGaSe 2 , CuInS 2 , CuInSe 2 , CuGaS 2 , CuGaSe 2 , CuAlS 2 and CuAlSe 2 . The new model calculations agree well with the results of Raman/IR and neutron measurements of Brillouin zone center phonon frequencies for both low and high frequency modes which was difficult for other phenomenological lattice dynamical models.

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Cited by 7 publications
(5 citation statements)
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“…The Raman analysis of CFS-1/2/3 was conducted, and the Raman spectra are presented in Figure b; the stronger peaks were located at 280/271/287 cm –1 in CFS-1/2/3, corresponding to the A 1 mode, and the peak at 469 cm –1 in CFS-1/3 was related to the E mode. The peaks at 212 and 211 cm –1 in CFS-1/2 were ascribed to the B 1 mode, and a weak peak at 349 cm –1 in CFS-3 corresponded to the B 2 mode, which were in good agreement with previous reports. It was obvious that the three samples had various vibrational modes, which may be concerned with particle sizes, but B 2 and E were polar Raman-active modes, showing transverse optical and longitudinal optical modes, which needed to be further investigated. The FT-IR analysis was applied to clarify the band, and the spectra are shown in Figure c.…”
Section: Results and Discussionsupporting
confidence: 88%
See 1 more Smart Citation
“…The Raman analysis of CFS-1/2/3 was conducted, and the Raman spectra are presented in Figure b; the stronger peaks were located at 280/271/287 cm –1 in CFS-1/2/3, corresponding to the A 1 mode, and the peak at 469 cm –1 in CFS-1/3 was related to the E mode. The peaks at 212 and 211 cm –1 in CFS-1/2 were ascribed to the B 1 mode, and a weak peak at 349 cm –1 in CFS-3 corresponded to the B 2 mode, which were in good agreement with previous reports. It was obvious that the three samples had various vibrational modes, which may be concerned with particle sizes, but B 2 and E were polar Raman-active modes, showing transverse optical and longitudinal optical modes, which needed to be further investigated. The FT-IR analysis was applied to clarify the band, and the spectra are shown in Figure c.…”
Section: Results and Discussionsupporting
confidence: 88%
“…The peaks at 212 and 211 cm −1 in CFS-1/2 were ascribed to the B 1 mode, and a weak peak at 349 cm −1 in CFS-3 corresponded to the B 2 mode, which were in good agreement with previous reports. 36−39 It was obvious that the three samples had various vibrational modes, which may be concerned with particle sizes, 35 but B 2 and E were polar Raman-active modes, showing transverse optical and longitudinal optical modes, 40 which needed to be further investigated. The FT-IR analysis was applied to clarify the band, and the spectra are shown in Figure 1c.…”
Section: Methodsmentioning
confidence: 99%
“…38 Semiempirical calculations based on the adiabatic bond charge model have also been published. 39 We display in Fig. 5 the phonon dispersion relations of CuGaX 2 (X = S, Se, Te) calculated by using the PBEsol approximation.…”
Section: Resultsmentioning
confidence: 99%
“…In terms of optical mode frequencies and symmetries our results are in very good agreement with those reported earlier in Refs. [9] and [10], but we benefited greatly from the analysis of vibrational patterns of selected modes, especially the only fully symmetric A 1 mode.…”
Section: Samples Experimental and Lattice Dynamics Calculationsmentioning
confidence: 99%
“…As already mentioned, apart from the crystallographic structure of mixed Ag x Ga x Ge 1− x Se 2 compounds, their nonlinear optical and photovoltaic properties, photoconductivity, and electronic band structure are well documented in the recent past . To the best of our knowledge, however, there are no reports on the transformation of phonon spectra of mixed Ag x Ga x Ge 1− x Se 2 crystals upon variation of composition x , despite of the fact that lattice dynamics properties of the end‐member compounds AgGaSe 2 and GeSe 2 were studied extensively both experimentally and theoretically. Probably, this is a consequence of a rather large unit cell of mixed crystals and, correspondingly, large number of expected phonon branches.…”
Section: Introductionmentioning
confidence: 99%