“…From measurements of the temperature dependence of librational parameters (Charbonneau & D61ugeard, 1976; and phonon frequencies (Plakida, Belushkin, Natkaniec & Watsiutynski, 1983), the model (~0)time=0 ° emerged as the best description of the hightemperature structure (HT structure) above 40 K. Between 40 and 17 K the HT b axis approximately doubles and the crystal shows incommensurate modulations in both the b* and a* directions (Cailleau, Moussa & Mons, 1979). At 17 K phase III appears in which the modulation in the a* direction has vanished, that along b* remains and the structure tends towards an ordering in space group Pa with Z = 4 but with q~ modulated between + 10 and -10 ° (Cailleau, Baudour & Zeyen, 1979;Baudour & Sanquer, 1983).…”