Abstract
An argument that relaxor ferroelectricity in the isovalent alloy can be understood as an induced moment soft pseudo-spin glass on the B-ions of the matrix is extended to the experimentally paradigmic but theoretically more complex heterovalent relaxor (PMN). It is argued that interesting behaviour of the onset of non-ergodicity, frequency-dependent susceptibility peaks and precursor nanodomains can be understood from analagous considerations of the B-ions, with the displacements of the Pb ions a largely independent, but distracting, side-feature. This contrasts with conventional conceptualizations.
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