Abstract
The Slater KDP model is solved for all temperatures and with an electric field. Above Tc the specific heat behaves lik (T−T c )−1/2 and the polarizability like (T−T c )−1. There is first-order phase transition at T c (latent heat). Below T c the free energy is simply -∣ℰ∣d (ℰ = electric field, d = dipole moment).
Work supported by National Science Foundation Grant No. GP-6851.
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Lieb, E.H. (2004). Exact Solution of the Two-Dimensional Slater KDP Model of a Ferroelectric. In: Nachtergaele, B., Solovej, J.P., Yngvason, J. (eds) Condensed Matter Physics and Exactly Soluble Models. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-06390-3_28
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DOI: https://doi.org/10.1007/978-3-662-06390-3_28
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