Phase transitions and H2O motions in ClO42 studied by infrared spectroscopy, inelastic/quasielastic incoherent neutron scattering and proton magnetic resonance Part II
Joanna Hetma?czyk; Anna Migda?-Mikuli; Edward Mikuli; Krystyna Ho?derna-Natkaniec; ?ukasz Hetma?czyk; Ireneusz Natkaniec
Journal of Molecular Structure 923(1-3): 103-109
2009
ISSN/ISBN: 0022-2860
DOI: 10.1016/j.molstruc.2009.02.009
Accession: 025228771
Fourier transform middle infrared spectroscopy, inelastic/quasielastic incoherent neutron scattering and proton magnetic resonance data for [Ca(H2O)4](ClO4)2 in the temperature range of 20–300 K and 110–300 K, respectively, are reported. Lack of infrared bands broadening with increasing temperature indicated that molecular reorientational correlation time is longer than 10−12 s. The elastic peak of neutron inelastic scattering registered in the high temperature phase shows broadening, which can be well described by a model of 180° instantaneous stochastic jumps of protons around the two-fold axis formed by the CaO bond, assuming that only two out of four H2O ligands per [Ca(H2O)4]2+ formula unit undergoes fast reorientation with reorientational correlation time R(H2O) of an order of 10−11 s. The analysis of the second moment M2 of 1H NMR line in the low temperature phase of [Ca(H2O)4](ClO4)2 revealed that the reorientation via 180° flips (jumps) of water molecules causes a very small changes of M2. It confirms that reorientation of H2O is fast even at 110 K. The reason for the first plateau of M2 ≈ 9.5 × 10−8 T2, which was observed at ca. 110–190 K range, is the anisotropic reorientation of whole [Ca(H2O)4]2+ cations around the two-fold symmetry axis going through two calcium atoms of the neighbouring [Ca(H2O)4]2+ cations. Above the phase transition at TC4h, the anisotropic reorientation of [Ca(H2O)4]2+ (around the pseudo three-fold symmetry axis formed by the Ca…O direction between [Ca(H2O)4]2+ cation and ClO4− anion, lying along the hydrogen bridge bond OH…O) is setting on with a frequency of the order of a few kHz, consequently above TC1h one can observe next plateau of M2 ≈ 2.5 × 10−8 T2.