Materials Science and Technology Division, Oak Ridge National Laboratory , Oak Ridge, Tennessee 37831, United States.
Department of Physics and Astronomy, University of Missouri , Columbia, Missouri 65211, United States.
ACS Nano. 2017 Nov 28;11(11):11617-11631. doi: 10.1021/acsnano.7b06640. Epub 2017 Nov 7.
Here we report a phase transition in H adsorbed in a locally graphitic Saran carbon with subnanometer pores 0.5-0.65 nm in width, in which two layers of hydrogen can just barely squeeze, provided they pack tightly. The phase transition is observed at 75 K, temperatures far higher than other systems in which an adsorbent is known to increase phase transition temperatures: for instance, H melts at 14 K in the bulk, but at 20 K on graphite because the solid H is stabilized by the surface structure. Here we observe a transition at 75 K and 77-200 bar: from a low-temperature, low-density phase to a high-temperature, higher density phase. We model the low-density phase as a monolayer commensurate solid composed mostly of para-H (the ground nuclear spin state, S = 0) and the high-density phase as an orientationally ordered bilayer commensurate solid composed mostly of ortho-H (S = 1). We attribute the increase in density with temperature to the fact that the oblong ortho-H can pack more densely. The transition is observed using two experiments. The high-density phase is associated with an increase in neutron backscatter by a factor of 7.0 ± 0.1. Normally, hydrogen produces no backscatter (scattering angle >90°). This backscatter appears along with a discontinuous increase in the excitation mass from 1.2 amu to 21.0 ± 2.3 amu, which we associate with collective nuclear spin excitations in the orientationally ordered phase. Film densities were measured using hydrogen adsorption. No phase transition was observed in H adsorbed in control activated carbon materials.
在这里,我们报告了在局部石墨化的 Saran 碳中吸附的 H 经历的一个相变,该 Saran 碳的纳米孔宽度为 0.5-0.65nm,刚好可以容纳两层氢原子,只要它们紧密排列。这种相变发生在 75K 的温度下,远高于其他已知可以提高相变温度的吸附剂系统:例如,在大块中 H 在 14K 熔化,但在石墨上因为固体 H 被表面结构稳定,所以在 20K 熔化。在这里,我们观察到在 75K 和 77-200bar 的相变:从低温、低密度相到高温、高密度相。我们将低密度相建模为主要由 para-H(基态核自旋态,S=0)组成的单层准固态,高密度相为主要由 ortho-H(S=1)组成的取向有序双层准固态。我们将密度随温度的增加归因于长形 ortho-H 可以更紧密地堆积的事实。该转变通过两个实验观察到。高密度相与中子背散射增加了 7.0±0.1 倍。通常,氢不会产生背散射(散射角>90°)。这种背散射与激发质量从 1.2amu 连续增加到 21.0±2.3amu 一起出现,我们将其与取向有序相中的集体核自旋激发相关联。通过氢吸附测量了薄膜密度。在对照活性炭材料中吸附的 H 中没有观察到相变。