首页> 外文期刊>Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics >Phase transitions and H_2O motions in [Ca(H_2O)_4](NO_3)_2 studied by infrared spectroscopy, inelastic/quasi-elastic incoherent neutron scattering and proton magnetic resonance, Part II
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Phase transitions and H_2O motions in [Ca(H_2O)_4](NO_3)_2 studied by infrared spectroscopy, inelastic/quasi-elastic incoherent neutron scattering and proton magnetic resonance, Part II

机译:红外光谱,非弹性/准弹性非相干中子散射和质子磁共振研究的[Ca(H_2O)_4](NO_3)_2中的相变和H_2O运动

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摘要

Fourier transform middle infrared spectroscopy (FT-MIR) inelastic/quasi-elastic incoherent neutron scattering (IINS/QENS) and proton magnetic resonance (~1H NMR) data for [Ca(H_2O)_4](NO_3)_2 in the temperature range of 20-300 K are reported. The temperature dependence of full width at half maximum (FWHM) of the infrared band (2v_(delta)(H_2O) mode) indicates that there exist a time (ps) fast re-orientational motions of H_2O ligands, with a mean value of activation energy of ca. 23 kJ mol~(-1), which is only slightly disturbed in the both phase transitions region. The elastic peak of neutron inelastic scattering, registered in the intermediate and high-temperature phase, shows broadening, which can be well described by a model of 180 deg instantaneous stochastic jumps of protons around the twofold axis formed by the Ca-O bond, assuming that only one out of four H_2O ligands per [Ca(H_2O)_4]~(2+) unit undergoes this fast reorientation. The ~1H NMR spin-lattice relaxation time T_1 decreases with increasing of temperature up to the phase transition temperature T_(C2)~h approx = 203 K and next starts drastically grows up till the room temperature, but in the meantime indicates small discontinuity at phase transition temperature T_(C1)~h approx = 244 K. The analysis of the second moment of ~1H NMR line in the low temperature phase of [Ca(H_2O)_4](NO_3)_2 revealed that the 180 deg flip of water molecules causes only very small changes of M_2. It was concluded that a reorientation of a whole [Ca(H_2O)_4]~(2+) cations (around the twofold symmetry axis going through two calcium atoms of the neighbouring [Ca(H_2O)_4]~(2+) cations) is the reason for the plateau of M_2 = 11.3 X 10~(-8) T~2 observed at ca. 100 K. Above the phase transition at T_(C2)~h, the anisotropic reorientation of [Ca(H_2O)_4]~(2+) (around the pseudo threefold symmetry axis going through two calcium atoms of the neighbouring [Ca(H_2O)_4]~(2+) cations) is set in motion with a frequency of the order of a few kilo hertz and just above 275 K one can observe a second plateau of M_2 = 3.0 X 10~(-8)T~2.
机译:[Ca(H_2O)_4](NO_3)_2的傅里叶变换中红外光谱(FT-MIR)非弹性/准弹性非相干中子散射(IINS / QENS)和质子磁共振(〜1H NMR)数据据报道20-300K。红外波段(2v_δ(H_2O)模式)的半峰全宽(FWHM)的温度依赖性表明存在H_2O配体快速重取向运动的时间(ps),具有激活平均值能量约23 kJ mol〜(-1),仅在两个相变区域中受到轻微干扰。假设在中高温阶段记录的中子非弹性散射的弹性峰变宽,可以用质子围绕由Ca-O键形成的双重轴的180度瞬时随机跃迁模型很好地描述。每个[Ca(H_2O)_4]〜(2+)单元中四个H_2O配体中只有一个经历了这种快速重新定向。 〜1H NMR自旋晶格弛豫时间T_1随温度的升高而降低,直至达到相变温度T_(C2)〜h约= 203 K,然后开始急剧增长直至室温,但同时表明在0相转变温度T_(C1)〜h约= 244K。对[Ca(H_2O)_4](NO_3)_2低温相中〜1H NMR线第二矩的分析表明,水翻转了180度分子仅引起很小的M_2变化。结论是,整个[Ca(H_2O)_4]〜(2+)阳离子发生了重新取向(绕着对称的对称轴穿过相邻的[Ca(H_2O)_4]〜(2+)阳离子的两个钙原子)的原因是在大约2时观测到M_2 = 11.3 X 10〜(-8)T〜2的平稳期。 100K。在T_(C2)〜h的相变之上,[Ca(H_2O)_4]〜(2+)的各向异性重新定向(围绕穿过相邻[Ca(H_2O)的两个钙原子的伪三重对称轴) )_4]〜(2+)阳离子)处于运动状态,频率约为几千赫兹,刚好高于275 K,可以观察到第二个平稳期M_2 = 3.0 X 10〜(-8)T〜2 。

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