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Facile Synthesis of LiH-Stabilized Face-Centered-Cubic YH3 High-Pressure Phase by Ball Milling Process

机译:通过球磨工艺容易合成LIH稳定的脸部中心立方YH3高压相

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摘要

A face-centered-cubic (FCC) YH3 phase is known to be stable only under high pressure (HP) of more than gigapascal order, and it reverts to the hexagonal YH3 ambient-pressure phase when the pressure is released. We previously found that the FCC YH3 can be stabilized even at ambient pressure by substituting Y for 10 mol % Li (LiH-stabilized YH3, LSY). The LSY was synthesized by heat treatment under gigapascal HP, but this process is unfavorable for mass production; that is, only a few tens of milligrams of a sample can be obtained in a single batch. In this study, we overcame this problem by applying a ball milling (BM) process for synthesizing the LSY phase, and the yield by the BM process reached on the order of grams. We confirmed that the structure of the BM sample was the same as that of the HP sample by X-ray diffractometry, Raman spectroscopy, and neutron total scattering pair distribution function analyses. The crystallinity of the BM sample, however, was lower than that of the HP sample. The difference in the crystallinity affects the thermal stability of the LSY. The BM sample with a lower crystallinity released hydrogen at a lower temperature. The BM sample was found to reversibly desorb/absorb hydrogen maintaining its initial FCC structure when the rehydrogenation temperature was at 423 K. However, when the rehydrogenation temperature of BM sample was more than 573 K, the FCC structure changed to the hexagonal ambient pressure phase due to thermal instability of FCC phase for the BM sample.
机译:已知朝向立方(FCC)YH3相仅在高于千兆卡斯卡级的高压(HP)下稳定,并且当压力被释放时,它恢复到六边形YH3环境压力阶段。我们以前发现,即使在环境压力下通过替代10mol%Li(LiH稳定的YH3,LSY),也可以稳定FCC YH3。 LSY通过千兆卡斯卡惠普下的热处理合成,但该过程对于大规模生产是不利的;也就是说,只有几十毫克样品可以在单批中获得。在这项研究中,我们通过施加球磨(BM)方法来克服该问题来合成LSY相,并且BM过程的产量达到克的顺序。我们证实,BM样品的结构与X射线衍射测定,拉曼光谱学和中子总散射对分布函数分析的HP样品的结构与HP样品相同。然而,BM样品的结晶度低于HP样品的结晶度。结晶度的差异影响了LSY的热稳定性。 BM样品具有下结晶度较低的氢气较低的温度。发现BM样品可逆地解吸/吸收氢气,在再氢化温度为423k时保持其初始FCC结构。然而,当BM样品的再氢化温度大于573K时,FCC结构变为六边形环境压力相由于BM样品的FCC阶段热不稳定性。

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