1998
DOI: 10.1143/jjap.37.5400
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Structural Phase Transitions in Zr-Rich Lead Zircon Titanate by Raman Scattering

Abstract: T h e method of Successive Linear Approximation at Maximum Steps, described in the previous paper, has been applied to automatic lens designing on an electronic digital computer. A description is given of the form of programme used and the results of applying the method to three design problems are quoted.

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Cited by 16 publications
(10 citation statements)
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“…The decreasing mode intensity with increasing temperature reflects a phase transition near 523 K. This mode has been associated with the anti-ferroelectric (orthorhombic) to ferroelectric (rhombohedral) phase transition at 507 K in PZ single crystal 73 and PbZr 0.95 Ti 0.05 O 3 ceramics. 74 The temperature-dependent micro-Raman results therefore confirm the intermediate ferroelectric phase in PZ films as observed in our polarization measurements.…”
Section: B-site Substitution In Pbtiosupporting
confidence: 87%
“…The decreasing mode intensity with increasing temperature reflects a phase transition near 523 K. This mode has been associated with the anti-ferroelectric (orthorhombic) to ferroelectric (rhombohedral) phase transition at 507 K in PZ single crystal 73 and PbZr 0.95 Ti 0.05 O 3 ceramics. 74 The temperature-dependent micro-Raman results therefore confirm the intermediate ferroelectric phase in PZ films as observed in our polarization measurements.…”
Section: B-site Substitution In Pbtiosupporting
confidence: 87%
“…This mode has been associated with the antiferroelectric ͑orthorhombic͒ to ferroelectric ͑rhombo-hedral͒ phase transition at 234°C in PZ single crystal 17 and PbZr 0.95 Ti 0.05 O 3 ceramics. 18 The low-frequency ( Ͻ100 cm Ϫ1 ) PZ modes are very sensitive to temperature and reflect a ferroelectric rhombohedral to paraelectric cubic phase at about 245°C in bulk material. 17,18 These modes were not resolved in the Raman spectra of the PZ films due to quasielastic scattering.…”
mentioning
confidence: 99%
“…18 The low-frequency ( Ͻ100 cm Ϫ1 ) PZ modes are very sensitive to temperature and reflect a ferroelectric rhombohedral to paraelectric cubic phase at about 245°C in bulk material. 17,18 These modes were not resolved in the Raman spectra of the PZ films due to quasielastic scattering. The changes near the rhombohedral to cubic phase transition temperature, therefore, are not distinct in the film spectra.…”
mentioning
confidence: 99%
“…This mode has been associated with the antiferroelectric ͑orthorhombic͒ to ferroelectric ͑rhombohedral͒ phase transition at 234°C in PZ single crystals 35 and PbZr 0.95 Ti 0.05 O 3 ceramics. 36 The lowfrequency (Ͻ100 cm Ϫ1 ) PZ modes are very sensitive to the temperature and reflect a ferroelectric rhombohedral to paraelectric cubic phase at about 245°C in bulk material. 35,36 These modes were not resolved in Raman spectra of the present set of La-modified PZ films due to the quasielastic scattering.…”
Section: Dielectric and Polarization Hysteresis Propertiesmentioning
confidence: 99%
“…36 The lowfrequency (Ͻ100 cm Ϫ1 ) PZ modes are very sensitive to the temperature and reflect a ferroelectric rhombohedral to paraelectric cubic phase at about 245°C in bulk material. 35,36 These modes were not resolved in Raman spectra of the present set of La-modified PZ films due to the quasielastic scattering. The changes near the rhombohedral to cubic phase-transition temperature, therefore, are not distinct in the film spectra.…”
Section: Dielectric and Polarization Hysteresis Propertiesmentioning
confidence: 99%