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