Elastic and magnetoelastic relaxation behaviour of multiferroic (ferromagnetic + ferroelectric + ferroelastic) Pb(Fe0.5Nb0.5)O3 perovskite
Creators
- 1. Department of Earth Sciences, University of Cambridge, Downing Street, Cambridge CB2 3EQ (United Kingdom)
- 2. National Physical Laboratory (CSIR), New Delhi 110012 (India)
- 3. Institute for Functional Nanomaterials, University of Puerto Rico, PO Box 23334, San Juan, 00931-3334 (Puerto Rico)
- 4. Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Strasse 40, 01187 Dresden (Germany)
- 5. Cavendish Laboratory, University of Cambridge, Madingley Road, Cambridge CB3 0HE (United Kingdom)
Description
Resonant Ultrasound Spectroscopy has been used to characterize elastic and anelastic anomalies in a polycrystalline sample of multiferroic Pb(Fe0.5Nb0.5)O3 (PFN). Elastic softening begins at ∼550 K, which is close to the Burns temperature marking the development of dynamical polar nanoregions. A small increase in acoustic loss at ∼425 K coincides with the value of T* reported for polar nanoregions starting to acquire a static or quasi-static component. Softening of the shear modulus by ∼30–35% through ∼395–320 K, together with a peak in acoustic loss, is due to classical strain/order parameter coupling through the cubic → tetragonal → monoclinic transition sequence of ferroelectric/ferroelastic transitions. A plateau of high acoustic loss below ∼320 K is due to the mobility under stress of a ferroelastic microstructure but, instead of the typical effects of freezing of twin wall motion at some low temperature, there is a steady decrease in loss and increase in elastic stiffness below ∼85 K. This is attributed to freezing of a succession of strain-coupled defects with a range of relaxation times and is consistent with a report in the literature that PFN develops a tweed microstructure over a wide temperature interval. No overt anomaly was observed near the expected Néel point, ∼145 K, consistent with weak/absent spin/lattice coupling but heat capacity measurements showed that the antiferromagnetic transition is actually smeared out or suppressed. Instead, the sample is weakly ferromagnetic up to ∼560 K, though it has not been possible to exclude definitively the possibility that this could be due to some magnetic impurity. Overall, evidence from the RUS data is of a permeating influence of static and dynamic strain relaxation effects which are attributed to local strain heterogeneity on a mesoscopic length scale. These, in turn, must have a role in determining the magnetic properties and multiferroic character of PFN. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/0953-8984/27/28/285901Additional details
Identifiers
Publishing Information
- Journal Title
- Journal of Physics. Condensed Matter
- Journal Volume
- 27
- Journal Issue
- 28
- Journal Page Range
- [18 p.]
- ISSN
- 0953-8984
- CODEN
- JCOMEL
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 47073533
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;
- Descriptors DEI
- ANTIFERROMAGNETISM; FERROELECTRIC MATERIALS; FLEXIBILITY; FREEZING; IMPURITIES; LOSSES; MAGNETIC PROPERTIES; MICROSTRUCTURE; MONOCLINIC LATTICES; ORDER PARAMETERS; PEROVSKITE; POLYCRYSTALS; SPECIFIC HEAT; SPECTROSCOPY; SPIN-LATTICE RELAXATION; STRAINS; STRESSES; TEMPERATURE RANGE 0065-0273 K; ULTRASONOGRAPHY
- Descriptors DEC
- CRYSTAL LATTICES; CRYSTAL STRUCTURE; CRYSTALS; DIAGNOSTIC TECHNIQUES; DIELECTRIC MATERIALS; DIMENSIONLESS NUMBERS; MAGNETISM; MATERIALS; MECHANICAL PROPERTIES; MINERALS; OXIDE MINERALS; PEROVSKITES; PHASE TRANSFORMATIONS; PHYSICAL PROPERTIES; RELAXATION; TEMPERATURE RANGE; TENSILE PROPERTIES; THERMODYNAMIC PROPERTIES; THREE-DIMENSIONAL LATTICES