2004
DOI: 10.1080/00150190490423417
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Elastic and Anelastic Properties of the Ceramics PbFe0.5Nb0.5O3: Anomalies NearTCandTN

Abstract: Low-frequency elastic and anelastic properties of the ceramic PbFe 0.5 Nb 0.5 O 3 were investigated by the inverted torsion pendulum in the temperature ranges including the Curie and Neel temperatures. Correlation between elastic and dielectric properties was found to take place within the diffuse ferroelectric phase transition. The shear modulus and the internal friction anomalies observed in the vicinity of T N are due to magnetostriction connection between a strain and magnetic spin ordering.

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Cited by 5 publications
(3 citation statements)
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“…Otherwise, it must be emphasized the value of θ c is smaller than θ ε , what is until now not clear. Similar difference was reported by O. N. Ivanov et al [15] that measured dielectric and elastic properties in PbFe 0.5 Nb 0.5 O 3 material.…”
Section: Resultssupporting
confidence: 91%
“…Otherwise, it must be emphasized the value of θ c is smaller than θ ε , what is until now not clear. Similar difference was reported by O. N. Ivanov et al [15] that measured dielectric and elastic properties in PbFe 0.5 Nb 0.5 O 3 material.…”
Section: Resultssupporting
confidence: 91%
“…PFN is a perovskite material in which, in general, the chemical formula (ABO 3 ) lead ions are located in positions A, while iron and niobium ions are located in octahedral positions B (alternatingly) [ 29 , 30 , 31 , 32 ]. PFN shows two ordered antiferromagnetic and ferroelectric subsystems (the magnetic phase transition takes place at about −130 °C temperature, whereas the ferroelectric phase transition occurs at about 110 °C temperature) [ 33 , 34 ]. PFN is used as a dielectric and magnetic medium for multi-layer ceramic condensers and coils, multi-layer ceramic capacitors (MLCC) and inductors, multi-layer microwave resonators and filters as tunable transducers, electrostriction actuators, servomotors, microcontrollers, sensors, detectors, and memory devices [ 35 , 36 , 37 , 38 , 39 , 40 , 41 , 42 ].…”
Section: Introductionmentioning
confidence: 99%
“…The PFN material is characterized by two ordered antiferromagnetic and ferroelectric subsystems. A change from the paramagnetic to ferroelectric phase takes place at about −130 • C temperature, whereas a change from the paraelectric to ferroelectric phase occurs at about 110 • C temperature [4,5].…”
Section: Introductionmentioning
confidence: 99%