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 | English (US) |
---|---|
Pages (from-to) | 108-110 |
Number of pages | 3 |
Journal | Physical review letters |
Volume | 19 |
Issue number | 3 |
DOIs | |
State | Published - 1967 |
All Science Journal Classification (ASJC) codes
- General Physics and Astronomy