Thoeny Alexander V, Parrichini Iside S, Gasser Tobias M, Loerting Thomas
Institute of Physical Chemistry, University of Innsbruck, Innrain 52c, A-6020 Innsbruck, Austria.
J Chem Phys. 2022 Apr 21;156(15):154507. doi: 10.1063/5.0087592.
The nature of the hydrogen substructure of a deuterated and deuterium chloride (DCI)-doped ice VI sample after cooling at 1.8 GPa has been a topic of recent interest-especially because the novel ice polymorph ice XIX was discovered in the course of such studies. We here investigate deuterated samples containing 5% HO using Raman spectroscopy to probe for transitions associated with rearrangement of D-atoms in ice XIX. The protocol involving heating at subambient pressure (10 mbar) in this study follows closely the one used in our earlier neutron diffraction study. Heating of ice XIX induces a complex cascade of processes involving both ordering and disordering of D atoms. Our Raman spectra demonstrate that the transition sequence is ice XIX → ice VI → ice XV, in accordance with our earlier neutron diffraction result. First signs for ice XIX decay are evident at 100 K, while ice XV build-up is seen only at 108 K and above. Between 100 and 108 K, a transiently disordered D-substructure appears, where at 108 K, ice VI forms from ice XIX and simultaneously decays to produce ice XV-thereby establishing a dynamic equilibrium. Using isothermal, time-resolved Raman spectroscopy in real time, we here determine rate constants, Avrami exponents, and activation energies for both slow processes, ice XIX decay and ice XV build-up. The first transition in this sequence, ice XIX decay, is faster than the second transition, ice XV build-up, so that ice VI accumulates. On the basis of the Johnson-Mehl-Avrami-Kolmogorov data obtained from the isothermal Raman experiment, we additionally report kinetic models for the development of fractions of ices XIX, XV, and VI in non-isothermal heating experiments at different heating rates. These models consider the two coupled first-order transitions as separated processes, where the phase fractions are calculated for incrementally small temperature (or time) steps. These models compare favorably with our previous observations for slowly or rapidly heated ice XIX samples, such as in calorimetry or neutron diffraction experiments.
在1.8 GPa下冷却后,氘化且掺杂氯化氘(DCl)的冰VI样品的氢亚结构性质一直是近期备受关注的话题,特别是因为在这类研究过程中发现了新型冰多晶型物——冰XIX。我们在此使用拉曼光谱研究含5% H₂O的氘化样品,以探测与冰XIX中D原子重排相关的转变。本研究中涉及在低于环境压力(10 mbar)下加热的实验方案与我们早期的中子衍射研究中使用的方案密切相关。冰XIX的加热引发了一系列复杂的过程,涉及D原子的有序化和无序化。我们的拉曼光谱表明,转变顺序为冰XIX→冰VI→冰XV,这与我们早期的中子衍射结果一致。冰XIX衰变的最初迹象在100 K时明显可见,而冰XV的形成仅在108 K及以上才能观察到。在100 K至108 K之间,出现了一个短暂无序的D亚结构,在108 K时,冰XIX形成冰VI,同时冰VI衰变产生冰XV,从而建立了动态平衡。我们在此使用实时等温、时间分辨拉曼光谱法,确定了冰XIX衰变和冰XV形成这两个缓慢过程的速率常数、阿弗拉米指数和活化能。该序列中的第一个转变,即冰XIX衰变,比第二个转变,即冰XV形成,要快,因此冰VI会积累。基于等温拉曼实验获得的约翰逊 - 梅尔 - 阿弗拉米 - 科尔莫戈罗夫数据,我们还报告了在不同加热速率的非等温加热实验中,冰XIX、XV和VI的分数发展的动力学模型。这些模型将这两个耦合的一级转变视为独立的过程,其中相分数是针对逐渐微小的温度(或时间)步长计算的。这些模型与我们之前对缓慢或快速加热的冰XIX样品的观察结果(如量热法或中子衍射实验中的观察结果)相比,具有良好的一致性。