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|
|Number of pages||3|
|Journal||Physical review letters|
|State||Published - Dec 1 1967|
ASJC Scopus subject areas
- Physics and Astronomy(all)