We show that very dilute concentrations of dipole impurities distributed in alkali halides (for example, OH^- impurities in KCl) undergo a phase transition provided that the average impurity-impurity interaction is greater than the tunnel-splitting energy of a single dipole. This theory predicts a temperature-dependent cusp in the dielectric constant. The polarization in the absence of an applied field is predicted to be zero even below the transition temperature.
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Fischer et al. (1976) studied this question.
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