Raman scattering in CaFeO3 and La0.33Sr0.67FeO3 across the charge-disproportionation phase transition

Ghosh, Shankar ; Kamaraju, N. ; Seto, M. ; Fujimori, A. ; Takeda, Y. ; Ishiwata, S. ; Kawasaki, S. ; Azuma, M. ; Takano, M. ; Sood, A. K. (2005) Raman scattering in CaFeO3 and La0.33Sr0.67FeO3 across the charge-disproportionation phase transition Physical Review B: Condensed Matter and Materials Physics, 71 (24). 245110_1-245110_7. ISSN 1098-0121

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Official URL: http://prb.aps.org/abstract/PRB/v71/i24/e245110

Related URL: http://dx.doi.org/10.1103/PhysRevB.71.245110

Abstract

Temperature-dependent micro-Raman studies of orthorhombic CaFeO3 and rhombohedral La0.33Sr0.67FeO3 were carried out with an aim to study the role of a lattice in the formation of the charge-disproportioned state (Fe4+→Fe5++Fe3+) below the transition temperature (Tco) of 290 and 200 K, respectively. Shell-model lattice-dynamical calculations were performed for CaFeO3 to assign the Raman modes and determine their vibrational pattern. The temperature dependence of the peak positions and the peak widths of various modes for both systems show distinct changes across their respective transition temperatures. In CaFeO3, the symmetric-stretching mode at 707 cm−1 splits into two modes, 707 cm−1 and 684 cm−1, corresponding to the breathing-type distortion of the FeO6 octahedra. In comparison, the spectral feature at 704 cm−1 in La0.33Sr0.67FeO3, which has been assigned to the Raman-forbidden symmetric-stretching mode, disappears below Tco. These observations indicate the presence of finite Jahn-Teller distortions of the FeO6 octahedra in CaFeO3 in the entire temperature range, whereas these distortions are present only above Tco in La0.33Sr0.67FeO3. Two modes at 307 cm−1 and 380 cm−1 in La0.33Sr0.67FeO3 approach each other at Tco, indicating a reduction of rhombohedral distortions below Tco.

Item Type:Article
Source:Copyright of this article belongs to American Physical Society.
ID Code:50245
Deposited On:22 Jul 2011 13:55
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