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氦在高压下如何以及为何会渗透过无孔的毒砂?

How and Why Does Helium Permeate Nonporous Arsenolite Under High Pressure?

作者信息

Guńka Piotr A, Hapka Michał, Hanfland Michael, Dranka Maciej, Chałasiński Grzegorz, Zachara Janusz

机构信息

Faculty of Chemistry, Warsaw University of Technology, Noakowskiego 3, 00-664, Warszawa, Poland.

Faculty of Chemistry, University of Warsaw, Pasteura 1, 02-093, Warszawa, Poland.

出版信息

Chemphyschem. 2018 Apr 5;19(7):857-864. doi: 10.1002/cphc.201701156. Epub 2018 Feb 13.

DOI:10.1002/cphc.201701156
PMID:29341365
Abstract

Investigations into the helium permeation of arsenolite, the cubic, molecular arsenic(III) oxide polymorph As O , were carried out to understand how and why arsenolite helium clathrate As O ⋅2 He is formed. High-pressure synchrotron X-ray diffraction experiments on arsenolite single crystals revealed that the permeation of helium into nonporous arsenolite depends on the time for which the crystal is subjected to high pressure and on the crystal history. The single crystal was totally transformed into As O ⋅2 He within 45 h under 5 GPa. After release of the pressure, arsenolite was recovered and a repeated increase in pressure up to 3 GPa led to practically instant As O ⋅2 He formation. However, when a pristine arsenolite single crystal was quickly subjected to a pressure of 13 GPa, no helium permeation was observed at all. No neon permeation was observed in analogous experiments. Quantum mechanical computations indicate that there are no specific attractive interactions between He atoms and As O molecules at the distances observed in the As O ⋅2 He crystal structure. Detailed analysis of As O molecular structure changes has shown that the introduction of He into the arsenolite crystal lattice significantly reduces molecular deformations by decreasing the anisotropy of stress exerted on the As O molecules. This effect and the pΔV term, rather than any specific As⋅⋅⋅He binding, are the driving forces for the formation As O ⋅2 He.

摘要

对立方晶系分子型三氧化二砷多晶型物毒砂(As₂O₃)的氦渗透进行了研究,以了解毒砂氦包合物As₂O₃·2He是如何形成以及为何形成的。对毒砂单晶进行的高压同步辐射X射线衍射实验表明,氦向无孔毒砂中的渗透取决于晶体承受高压的时间以及晶体的历史。在5 GPa下,单晶在45小时内完全转变为As₂O₃·2He。压力释放后,毒砂得以恢复,再次将压力升高至3 GPa会导致几乎瞬间形成As₂O₃·2He。然而,当将原始的毒砂单晶迅速施加13 GPa的压力时,根本未观察到氦的渗透。在类似实验中也未观察到氖的渗透。量子力学计算表明,在As₂O₃·2He晶体结构中观察到的距离下,He原子与As₂O₃分子之间不存在特定的吸引相互作用。对As₂O₃分子结构变化的详细分析表明,将He引入毒砂晶格中可通过降低施加在As₂O₃分子上的应力各向异性来显著减少分子变形。这种效应和pΔV项,而非任何特定的As···He键合,是形成As₂O₃·2He的驱动力。

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