Uniaxial ferroelectrics with tetragonal tungsten bronze structure are important functional materials with photorefractive, electrooptic, piezoelectric, and pyroelectric properties. SrBaNbO (SBN100) with > 50 is known as a typical uniaxial relaxor ferroelectric, while CaBaNbO (CBN100) undergoes nearly normal ferroelectric phase transitions. Single crystals of CSBN100 = [(CBN28) + (1 - ) (SBN61)] = CaBaNbO + (1 - ) SrBaNbO with nominal = 0.
View Article and Find Full Text PDFBoth relaxor ferroelectric and antiferroelectric materials can individually demonstrate large electrocaloric effects (ECE). However, in order to further enhance the ECE it is crucial to find a material system, which can exhibit simultaneously both relaxor ferroelectric and antiferroelectric properties, or easily convert from one into another in terms of the compositional tailoring. Here we report on a system, in which the structure can readily change from antiferroelectric into relaxor ferroelectric and vice versa.
View Article and Find Full Text PDFFerrimagnetic CoFe2O4 nanopillars embedded in a ferroelectric BaTiO3 matrix are an example for a two-phase magnetoelectrically coupled system. They operate at room temperature and are free of any resource-critical rare-earth element, which makes them interesting for potential applications. Prior studies succeeded in showing strain-mediated coupling between the two subsystems.
View Article and Find Full Text PDFIEEE Trans Ultrason Ferroelectr Freq Control
October 2010
Magnetoelectric (ME) materials are of utmost interest in view of both fundamental understanding and novel desirable applications. Despite its smallness, the linear ME effect has been shown to control spintronic devices very efficiently, e.g.
View Article and Find Full Text PDFIEEE Trans Ultrason Ferroelectr Freq Control
December 2006
The evolution of the nanodomain pattern of the uniaxial relaxor ferroelectric strontium barium niobate doped with cerium was studied by piezoresponse force microscopy (PFM). The fractal-like nanodomains observed at room temperature decay on heating. At temperatures up to about 15 K above the Curie temperature, Tc = 320 K, areas of correlated polarization are still visible.
View Article and Find Full Text PDFThe charge-disordered three-dimensional uniaxial relaxor ferroelectric Sr0.61Ba0.39Nb2O6 splits up into metastable polar nanoregions and paraelectric interfaces upon cooling from above Tc.
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