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Phase Transition of H-2 in Subnanometer Pores Observed at 75 K

机译:在75 k观察到亚腔轮孔中H-2的相转变

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Here we report a phase transition in H-2 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-2 melts at 14 K in the bulk, but at 20 K on graphite because the solid H-2 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-2 (the ground nuclear spin state, S = 0) and the high-density phase as an orientationally ordered bilayer commensurate solid composed mostly of ortho-H-2 (S = 1). We attribute the increase in density with temperature to the fact that the oblong ortho-H-2 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 degrees). 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-2 adsorbed in control activated carbon materials.
机译:在这里,我们在宽度的亚脑仪孔中报告了吸附在局部石墨砂碳中的相转变,其中两层氢可勉强挤压,只要它们紧紧地包装。在75 k处观察到相转变,温度远远高于已知吸附剂增加相转变温度的其他系统:例如,H-2在块状的14k下熔化,但是在石墨上以20 k处于石墨,因为固体H-2通过表面结构稳定。在这里,我们观察到75 k和77-200栏的过渡:从低温,低密度相到高温,更高的密度相。我们将低密度相模型为单层相称的固体,主要由Para-H-2(地面核旋转状态,S = 0)和高密度相位,作为主要有序的双层相称固体,主要由Ortho-H组成-2(s = 1)。我们将密度的增加与温度归因于椭圆形Ortho-H-2可以更密集地包装的事实。使用两个实验观察到过渡。高密度相与中子反向散射的增加有关,倍数为7.0 +/- 0.1。通常,氢不产生反向散射(散射角> 90度)。这种反向散射随着从1.2 AMU到21.0 +/- 2.3 AMU的激励质量的不连续增加,我们在定义有序的阶段与集体核自旋激发联系起来。使用氢吸附测量胶片密度。在吸附于对照活性炭材料的H-2中没有观察到相转变。

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