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Guest-free monolayer clathrate and its coexistence with two-dimensional high-density ice

机译:无客体的单层包合物及其与二维高密度冰的共存

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摘要

Three-dimensional (3D) gas clathrates are ice-like but distinguished from bulk ices by containing polyhedral nano-cages to accommodate small gas molecules. Without space filling by gas molecules, standalone 3D clathrates have not been observed to form in the laboratory, and they appear to be unstable except at negative pressure. Thus far, experimental evidence for guest‐free clathrates has only been found in germanium and silicon, although guest‐free hydrate clathrates have been found, in recent simulations, able to grow from cold stretched water, if first nucleated. Herein, we report simulation evidence of spontaneous formation of monolayer clathrate ice, with or without gas molecules, within hydrophobic nano-slit at low temperatures. The guest-free monolayer clathrate ice is a low-density ice (LDI) whose geometric pattern is identical to Archimedean 4·82-truncated square tiling, i.e. a mosaic of tetragons and octagons. At large positive pressure, a second phase of 2D monolayer ice, i.e. the puckered square high-density ice (HDI) can form. The triple point of the LDI/liquid/HDI three-phase coexistence resembles that of the ice-Ih/water/ice-III three-phase coexistence. More interestingly, when the LDI is under a strong compression at 200 K, it transforms into the HDI via a liquid intermediate state, the first direct evidence of Ostwald’s rule of stages at 2D. The tensile limit of the 2D LDI and water are close to that of bulk ice-Ih and laboratory water.
机译:三维(3D)气体包合物像冰一样,但与散装冰不同,它包含多面体纳米笼以容纳较小的气体分子。没有由气体分子填充的空间,在实验室中未观察到形成独立的3D笼形物,除了负压外,它们似乎不稳定。迄今为止,虽然在无铅水合物中发现了无客体的水合物,但在最近的模拟中,如果先形成核后,它们就可以从冷拉伸水中生长,但到目前为止,仅在锗和硅中发现了无客体水合物的实验证据。在本文中,我们报告了在低温下在疏水性纳米缝隙内自发形成单层笼形冰的模拟证据,有或没有气体分子。无客体的单层笼形冰是一种低密度冰(LDI),其几何图案与阿基米德4×8 2 截短的正方形瓷砖相同,即四边形和八边形的马赛克。在大正压力下,可以形成2D单层冰的第二相,即起皱的方形高密度冰(HDI)。 LDI /液体/ HDI三相共存的三相类似于冰-Ih /水/冰III三相共存的三相。更有趣的是,当LDI在200 K下受到强烈压缩时,它会通过液态中间状态转变为HDI,这是奥斯特瓦尔德在2D阶段的阶段规则的直接证据。 2D LDI和水的拉伸极限接近于大体积冰-Ih和实验室用水的拉伸极限。

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