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Nb-H system at high pressures and temperatures

机译:NB-H系统高压和温度

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摘要

We studied the Nb-H system over extended pressure and temperature ranges to establish the highest level ofhydrogen abundancewe could achieve from the resulting alloy.We probed the Nb-H system with laser heating andx-ray diffraction complemented by numerical density functional theory-based simulations. New quenched doublehexagonal close-packed (hcp) NbH_(2.5) appears under 46 Gpa, and above 56 Gpa cubic NbH3 is formed as theoreticallypredicted. Nb atoms are arranged in close-packed lattices which are martensitically transformed in the sequence:face-centered cubic (fcc)→hcp→double hcp (dhcp)→distorted body-centered cubic (bcc) as pressureincreases. The appearance of fcc NbH_(2.5−3) and dhcp NbH_(2.5) cannot be understood in terms of enthalpic stability,but can be rationalized when finite temperatures are taken into account. The structural and compressional behaviorof NbH_(x>2) is similar to that of NbH. Nevertheless, a direct H-H interaction emerges with hydrogen concentrationincreases, which manifests itself via a reduction in the lattice expansion induced by hydrogen dissolution.
机译:我们研究了NB-H系统的扩展压力和温度范围,以确定最高水平氢丰度机可以从所得合金中实现。我们用激光加热探测NB-H系统基于数值函数理论的模拟互补的X射线衍射。新的淬火双倍六边形近填充(HCP)NbH_(2.5)出现在46GPa以下,在理论上形成56 GPA立方NBH3预料到的。 Nb原子布置在近封装的晶格中,在序列中是马持的:面向中心的立方(FCC)→HCP→双HCP(DHCP)→扭曲的身体中心立方(BCC)作为压力增加。在焓稳定方面,不能理解FCC NBH_(2.5-3)和DHCP NBH_(2.5)的外观,但是当考虑有限气温时,可以合理化。结构和压缩行为nbh_(x> 2)类似于nbh的nbh。然而,直接H-H相互作用随氢浓度出现增加,通过减少氢溶解诱导的晶格扩张的减少来表现出来。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第10期|104110.1-104110.9|共9页
  • 作者单位

    State Key Laboratory of Superhard Materials Department of Physics Jilin University Changchun 130012 China Max Planck Institute for Chemistry Mainz 55020 Germany National Key Laboratory of Shock Wave and Detonation Physics Institute of Fluid Physics China Academy of Engineering Physics Mianyang 621900 China;

    Max Planck Institute for Chemistry Mainz 55020 Germany;

    National Research Centre “Kurchatov Institute ” Moscow Russia;

    Geophysical Laboratory Carnegie Institution of Washington Washington DC 20015 USA;

    State Key Laboratory of Metastable Materials Science and Technology Yanshan University Qinhuangdao 066004 China;

    Max Planck Institute for Chemistry Mainz 55020 Germany;

    State Key Laboratory of Superhard Materials Department of Physics Jilin University Changchun 130012 China;

    State Key Laboratory of Superhard Materials Department of Physics Jilin University Changchun 130012 China International Center of Future Science Jilin University Changchun 130012 China;

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