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• W4236478889 abstract "Disordered multiferroic materials ( type-III multiferroics ) escape the conventional schematics of type-I and type-II multiferroics, where two types of ferroic long-range order are expected to coexist under different interdependences and promise to attain a maximized bilinear ( α or EH ) magnetoelectric effect under special symmetry conditions. Nevertheless sizable higher order ME response occurs also in disordered systems such as in the simultaneous dipolar and spin glasses ( multiglass ) Sr 0.98 Mn 0.02 TiO 3 and K 0.94 Mn 0.03 TaO 3 , the quantum paraelectric antiferromagnet EuTiO 3 , the spin glass and relaxor ferroelectric PbFe 0.5 Nb 0.5 O 3 , and the antiferroelectric antiferromagnetic dipole glass CuCr 1-x In x P 2 S 6 . They have in common to show large quadratic magneto-capacitance effects, Δε H 2 , which are related to dominating third-order E 2 H 2 terms in their free energies and do not require special symmetry conditions. The polarization controlled exchange coupling can achieve giant fluctuation-enhanced values in the vicinity of critical magnetic fields as observed, e.g. , in EuTiO 3 . Exceptionally, even the first-order EH -type magnetoelectric effect is observed whenever metastable homogeneous order parameters are induced by field cooling as in EuTiO 3 , or in the spin glass phase of the relaxor multiferroic Pb (Fe 0.5 Nb 0.5 )O 3 at T < T g = 10.6 K." @default.
• W4236478889 created "2022-05-12" @default.
• W4236478889 creator A5043832976 @default.
• W4236478889 date "2012-06-01" @default.
• W4236478889 modified "2023-09-26" @default.
• W4236478889 title "Disordered Multiferroics" @default.
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• W4236478889 doi "https://doi.org/10.4028/www.scientific.net/ssp.189.41" @default.
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