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首页> 外文期刊>Journal of Applied Physics >Experimental and theoretical characterization of ordered MAX phases Mo_2TiAlC_2 and Mo_2Ti_2AlC_3
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Experimental and theoretical characterization of ordered MAX phases Mo_2TiAlC_2 and Mo_2Ti_2AlC_3

机译:有序MAX相Mo_2TiAlC_2和Mo_2Ti_2AlC_3的实验和理论表征

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Herein, we report on the phase stabilities and crystal structures of two newly discovered ordered, quaternary MAX phases-Mo_2TiAlC_2 and Mo_2Ti_2AlC_3-synthesized by mixing and heating different elemental powder mixtures of mMo:(3-m)Ti:1.1Al:2C with 1.5≤m≤2.2 and 2Mo: 2Ti:1.1Al:2.7C to 1600℃ for 4h under Ar flow. In general, for m≥2 an ordered 312 phase, (Mo_2Ti)AlC_2, was the majority phase; for m<2, an ordered 413 phase (Mo_2Ti_2)AlC_3, was the major product. The actual chemistries determined from X-ray photoelectron spectroscopy (XPS) are Mo_2TiAlC_(1.7) and Mo_2Ti_(1.9)Al_(0.9)C_(2.5), respectively. High resolution scanning transmission microscopy, XPS and Rietveld analysis of powder X-ray diffraction confirmed the general ordered stacking sequence to be Mo-Ti-Mo-Al-Mo-Ti-Mo for Mo_2TiAlC_2 and Mo-Ti-Ti-Mo-Al-Mo-Ti-Ti-Mo for Mo_2Ti_2AlC_3, with the carbon atoms occupying the octahedral sites between the transition metal layers. Consistent with the experimental results, the theoretical calculations clearly show that M layer ordering is mostly driven by the high penalty paid in energy by having the Mo atoms surrounded by C in a face-centered configuration, i.e., in the center of the M_(n+1)X_n blocks. At 331 GPa and 367 GPa, respectively, the Young's moduli of the ordered Mo_2TiAlC_2 and Mo_2Ti_2AlC_3 are predicted to be higher than those calculated for their ternary end members. Like most other MAX phases, because of the high density of states at the Fermi level, the resistivity measurement over 300 to 10 K for both phases showed metallic behavior.
机译:在此,我们报告了通过将mMo:(3-m)Ti:1.1Al:2C与1.5的不同元素粉末混合物混合并加热而合成的两个新发现的有序四元MAX相-Mo_2TiAlC_2和Mo_2Ti_2AlC_3-的相稳定性和晶体结构。 ≤m≤2.2且2Mo:2Ti:1.1Al:2.7C在氩气流下于1600℃放置4h。通常,对于m≥2,有序的312相(Mo_2Ti)AlC_2是多数相。对于m <2,主要产物是有序413相(Mo_2Ti_2)AlC_3。由X射线光电子能谱(XPS)确定的实际化学分别为Mo_2TiAlC_(1.7)和Mo_2Ti_(1.9)Al_(0.9)C_(2.5)。高分辨率扫描透射显微镜,XPS和粉末X射线衍射的Rietveld分析证实,对于Mo_2TiAlC_2和Mo-Ti-Ti-Mo-Al-Mo-,Mo-Ti-Mo-Al-Mo-Ti-Mo的一般有序堆积顺序为Mo_2Ti_2AlC_3的Mo-Ti-Ti-Mo,碳原子占据过渡金属层之间的八面体位置。与实验结果一致,理论计算清楚地表明,M层有序主要是由Mo原子以面心为中心(即M_(n +1)X_n个区块。预测在有序Mo_2TiAlC_2和Mo_2Ti_2AlC_3的杨氏模量分别为331 GPa和367 GPa时,其杨氏模量要高于为其三元末端成员计算的杨氏模量。像大多数其他MAX相一样,由于费米能级的状态密度很高,因此两相在300至10 K范围内的电阻率测量都显示出金属行为。

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  • 来源
    《Journal of Applied Physics 》 |2015年第9期| 094304.1-094304.14| 共14页
  • 作者单位

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA,A.J. Drexel Nanomaterials Institute, Drexel University, Philadelphia, Pennsylvania 19104, USA;

    Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA,Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA;

    Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA,Physics Department, Nuclear Research Centre - Negev, PO Box 9001, 84190 Beer-Sheva, Israel;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA;

    Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Thin Film Physics Division, Department of Physics, Chemistry and Biology (IFM), Linkoeping University, SE-581 83 Linkoeping, Sweden;

    Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA;

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