1983 年 52 巻 10 号 p. 3475-3485
The heat capacity of Rb2ZnBr4 was measured from 3 to 300 K. The commensurate-incommensurate phase transition (so-called lock-in transition) showed very small anomaly of the first-order at (193.6±0.3) K with ΔHt=(9.3±1.0) J·mol−1 and ΔSt=(0.048±0.005) J·K−1·mol−1. Below the lock-in transition, two phase transitions were observed. A typical second-order anomaly was at (111.7±0.2) K with ΔHt=(47±5) J·mol−1 and ΔSt=(0.45±0.05) J·K−1·mol−1. Another anomaly was observed at (76.5±0.1) K with ΔHt=(2.0±0.3) J·mol−1 and ΔSt=(0.027±0.004) J·K−1·mol−1. A unified treatment of the successive transitions in K2SeO4, Rb2ZnCl4, and Rb2ZnBr4 is given based on a Landau-type phenomenological theory. Numerical calculation of heat capacities and entropies of the lock-in transitions showed general agreement with the experimental results.
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