1984
DOI: 10.1088/0022-3719/17/3/020
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Infrared spectroscopy in KNbO3through the successive ferroelectric phase transitions

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Cited by 245 publications
(135 citation statements)
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“…Similar calculations have been done earlier by other methods, 5,6,8 and the experimental data (obtained mostly by infrared reflectivity measurements 32,33 ) are available. We performed the calculations for a lattice constant a = 3.997Å (that is based on an experimental perovskite cell volume extrapolated to zero temperature) within a conventional frozen-phonon scheme, using the 2 × 2 × 2 LUC.…”
Section: B γ-To Frozen Phonons In the Cubic Phasesupporting
confidence: 54%
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“…Similar calculations have been done earlier by other methods, 5,6,8 and the experimental data (obtained mostly by infrared reflectivity measurements 32,33 ) are available. We performed the calculations for a lattice constant a = 3.997Å (that is based on an experimental perovskite cell volume extrapolated to zero temperature) within a conventional frozen-phonon scheme, using the 2 × 2 × 2 LUC.…”
Section: B γ-To Frozen Phonons In the Cubic Phasesupporting
confidence: 54%
“…The general symmetry relations between the Γ phonon modes in the cubic and rhombohedral phases may be found, e.g., in Ref. 32. We consider in the present work only three A 1 modes, which originate from the T 1u block of the cubic phase, as the crystal symmetry lowers and all the soft modes become stabilized.…”
Section: Displacements and Phonons In The Rhombohedral Phasementioning
confidence: 91%
“…In this same work the Berry-phase theory of macroscopic polarization [5,6] is implemented within the HF scheme, using first-principles ingredients. Perhaps the most interesting result that has emerged is that the calculated HF spontaneous polarization of KNbO 3 in its tetragonal phase is 0.34 C/m 2 , quite close to the experimental value [7], which is 0.37 C/m 2 , as well as previous LDA results [8][9][10], which are between 0.33 and 0.40 C/m 2 .…”
Section: Introductionsupporting
confidence: 84%
“…These modes are classified into three phonon bands which corresponds to normal modes of the ideal cubic perovskite: external modes (ω < 290 cm −1 ), bending mode at the intermediate range, and stretching modes (ω > 550 cm −1 ). The low frequency external modes are due to the vibrations of R and MnO 6 , while the intermediate frequency range bending modes and the high frequency stretching modes mainly involve vibrations of oxygen octahedra [20]. Hence, the modes assignment will be made by comparing the phonon frequencies obtained from the fit with those found in lattice dynamics calculations [17,24] as given in Table II.…”
Section: Resultsmentioning
confidence: 99%