Fortes A Dominic
ISIS Facility, STFC Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Chilton, Oxfordshire OX11 0QX, UK.
Acta Crystallogr B Struct Sci Cryst Eng Mater. 2018 Apr 1;74(Pt 2):196-216. doi: 10.1107/S2052520618002159. Epub 2018 Mar 20.
Accurate and precise lattice parameters for DO and HO varieties of hexagonal ice (ice Ih, space group P6/mmc) have been obtained in the range 1.6 to 270 K. Precision of the lattice parameters (∼0.0002% in a and 0.0004% in c for DO, 0.0008% in a and 0.0015% in c for HO) is ensured by use of the time-of-flight method on one of the longest primary neutron flight-path instruments in the world, the High-Resolution Powder Diffractometer at the ISIS neutron source. These data provide a more precise description of the negative thermal expansion of the material at low temperatures than the previous synchrotron gold standard' [Röttger et al. (1994). Acta Cryst. B50, 644-648], including the region below 10 K where the lattice parameters saturate. The volume expansivity of both isotopologues turns negative below 59-60 K, in excellent agreement with a recent dilatometry study. The axial expansivities are highly isotropic (differing by < 1% in DO ice Ih). Furthermore, the c/a ratio of different DO ice samples exhibit a statistically significant dispersion of ∼0.015% below 150 K that appears to depend on the thermal history of the sample, which disappears on warming above 150 K. Similarly, HO ice exhibits a kink' in the c/a ratio at ∼115 K. The most plausible explanation is a freezing-in of the molecular reorientation process on cooling and subsequent relaxation on warming.
已获得六方冰(冰Ih,空间群P6/mmc)的DO和HO变体在1.6至270 K范围内准确且精确的晶格参数。通过使用世界上最长的一次中子飞行路径仪器之一——ISIS中子源的高分辨率粉末衍射仪上的飞行时间方法,确保了晶格参数的精度(DO的a精度约为0.0002%,c精度约为0.0004%;HO的a精度约为0.0008%,c精度约为0.0015%)。这些数据比之前的同步加速器“黄金标准”[Röttger等人(1994年)。《晶体学报》B50,644 - 648]更精确地描述了该材料在低温下的负热膨胀情况,包括晶格参数饱和的10 K以下区域。两种同位素变体的体积膨胀系数在59 - 60 K以下变为负值,这与最近的膨胀测量研究结果非常吻合。轴向膨胀系数具有高度各向同性(DO冰Ih中相差<1%)。此外,不同DO冰样品的c/a比在150 K以下表现出约0.015%的统计学显著分散,这似乎取决于样品的热历史,在温度升至150 K以上时这种分散消失。同样,HO冰在约115 K时c/a比出现“扭结”。最合理的解释是分子重排过程在冷却时被冻结,随后在升温时松弛。