V. Rodriguez et al., INCOHERENT QUASI-ELASTIC NEUTRON-SCATTERING STUDY OF N(CH3)(4)MNCL3(TMMC), Journal of physical chemistry, 100(33), 1996, pp. 14109-14117
Crystalline N(CH3)(4)MnCl3 (TMMC) exhibits a phase transition at T-c =
126 K from a high-temperature hexagonal phase, where the [N(CH3)(4)](
+) (TMA) groups are orientationally disordered, to a low-temperature-o
rdered monoclinic phase. Incoherent quasielastic neutron scattering (I
QNS) experiments were performed in order to investigate the reorientat
ional dynamics of the TMA in both phases. The IQNS profiles, obtained
on a medium resolution time-of-flight instrument (approximate to 110 m
u eV) for the hexagonal phase and on a higher resolution spectrometer
(approximate to 33 mu eV) for the monoclinic phase, were analyzed in t
he 305-145 and 100-60 K temperature ranges, respectively. A model has
been proposed in which the TMA cations are in instantaneous general or
ientation so that each methyl group can probe 24 equivalent sites in t
he hexagonal phase. This model involves three basic reorientational mo
tions of the cation. The first one is a precession of TMA around the 3
-fold crystallographic axis, which slows down very quickly with decrea
sing temperature and can be no longer resolved below 200 K. The second
one corresponds to a rotation of the cation about the 3-fold crystall
ographic axis. In the hexagonal phase, the third motion (flip), which
is connected to the crystallographic mirror plane, is by far the faste
r one (characteristic time around 1 ps at 300 K). In the monoclinic ph
ase, the thermal evolution of the IQNS profiles is essentially interpr
eted by a progressive freezing of the flip motion between two inequiva
lent orientations of the TMA (loss of the crystallographic mirror plan
e) as the temperature decreases. These results are then discussed in t
he context of the mechanism of phase transitions occurring in TMMC.