Answers are grounded in this paper and cite their sources.
A pseudo-spin model of a KDP-type ferroelectric is assumed to have strain-dependence in both exchange coupling and tunnelling. A self-consistent molecular field calculation is made of both the polarization and the expectation (X) of the spin-flip operator, for T<T c . In the case of a model with one spin per cell, it is shown that there can never be a second-order phase change when piezoelectric coupling is finite, and that T c to 0K if the coefficient Gamma 1 of strain- dependence of tunnelling is made sufficiently large. A small Gamma 1 is found to augment effects produced by changes in the strain-independent part Gamma 0 of the tunnelling. In the case of zero piezoeffect, an increase in Gamma 1 can reduce the transition from first- to second-order, while small ranges of Gamma 1 values are found within which it is impossible to make T c to 0 as Gamma 0 increases. A two-sublattice model is discussed, in which sublattice polarization can differ for H bonds of differing orientation. Again, for Gamma 1 sufficiently large, the ferroelectric phase disappears.
No takes yet. Share an insight, caveat, or question.
R. E. Nettleton (1975) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: