Abstract
The Slater KDP model is solved for all temperatures and with an electric field. Above Tc the specific heat behaves like (T-Tc)-12 and the polarizability like (T-Tc)-1. There is a first-order phase transition at Tc (latent heat). Below Tc the free energy is simply -|E|d (E=electric field, d=dipole moment).
Original language | American English |
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Pages (from-to) | 108-110 |
Number of pages | 3 |
Journal | Physical review letters |
Volume | 19 |
Issue number | 3 |
DOIs | |
State | Published - Dec 1 1967 |
ASJC Scopus subject areas
- Physics and Astronomy(all)