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Nanoscale heterogeneity, premartensitic nucleation, and a new plutonium structure in metastable δ fcc Pu-Ga alloys

机译:亚稳态δfcc Pu-Ga合金的纳米级异质性,马氏体形核和新的p结构

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摘要

The scientifically fascinating question of the spatial extent and bonding of the 5 f orbitals of Pu and its six different phases extends to its δ-retained alloys and the mechanism by which Ga and a number of other unrelated elements stabilize its low density face-centered-cubic (fcc) structure. This issue of phase stability is also important technologically because of its significance to Science-Based Stockpile Stewardship. Answering these questions requires information on the local order and structure around the Ga and its effects on the Pu. We have addressed this by characterizing the structures of a large number of Pu-Ga and two Pu-In and one Pu-Ce δ alloys, including a set of high purity δ Pu_(1-x)Ga_x materials with 1.7 ≤x≤6.4 at. % Ga that span the low [Ga] portion of the δ region of the phase diagram across the ~3.3 at. % Ga metastability boundary, with extended x-ray absorption fine structure (EXAFS) spectroscopy that probes the element specific local structure, supplemented by x-ray pair distribution function analysis that gives the total local structure to longer distances, and x-ray diffraction that gives the long-range average structure of the periodic component of the materials. Detailed analyses indicate that the alloys at and below a nominal composition of ~3.3 at. % Ga are heterogeneous and in addition to the δ phase also contain up to ~20% of a novel, coexisting "σ" structure for Pu that forms in nanometer scale domains that are locally depleted in Ga. The invariance of the Ga EXAFS with composition indicates that this σ structure forms in Ga-depleted domains that result from the Ga atoms in the δ phase self-organizing into a quasi-intermetallic with a stoichiometry of Pu_(25-35)Ga so that δ Pu-Ga is neither a random solid solution nor the more stable Pu_3Ga + α. Above this 3.3 at. % Ga nominal composition, the δ Pu-Ga alloy is homogeneous, and no σ phase is present. These results that demonstrate that collective and cooperative behavior in the interactions between the alloy elements as well as local elastic forces are crucial in determining the properties of complex materials and contradict the conventional mechanism for martensitic transformations, in this case indicating that nucleation is not the rate limiting step.
机译:Pu的5f轨道及其六个不同相的空间范围和键合的科学迷人问题扩展到其δ保留合金,以及Ga和许多其他不相关元素稳定其低密度面心合金的机制。立方(FCC)结构。由于其对基于科学的储备管理具有重要意义,因此相位稳定性问题在技术上也很重要。要回答这些问题,就需要有关Ga附近的局部秩序和结构及其对Pu的影响的信息。我们通过表征大量Pu-Ga和两种Pu-In和一种Pu-Ceδ合金的结构来解决此问题,包括一系列1.7≤x≤6.4的高纯度δPu_(1-x)Ga_x材料。在。 %Ga横跨相图δ区的低[Ga]部分,跨度为〜3.3 at。 %Ga亚稳性边界,具有扩展的X射线吸收精细结构(EXAFS)光谱学,可探测元素特定的局部结构,并辅之以X射线对分布函数分析,可将整个局部结构延伸到更长的距离,并进行X射线衍射给出了材料的周期性成分的远程平均结构。详细的分析表明,合金的标称成分在或低于〜3.3 at。 %Ga是异质的,除δ相外,还包含高达〜20%的Pu新型共存“σ”结构,该结构在Ga局部耗尽的纳米级域中形成。Ga EXAFS随组成的不变性表明这种σ结构形成在Ga贫化区中,这是由于δ相中的Ga原子自组织为化学计量为Pu_(25-35)Ga的准金属间化合物,因此δPu-Ga既不是随机的固溶体也不是更稳定的Pu_3Ga +α。高于此3.3 at。以Ga名义组成为准,δPu-Ga合金是均匀的,没有σ相。这些结果表明,合金元素之间相互作用中的集体和协作行为以及局部弹性力对于确定复杂材料的性能至关重要,并且与马氏体相变的常规机理相矛盾,在这种情况下,表明成核不是速率限制步骤。

著录项

  • 来源
    《Physical review》 |2014年第22期|224102.1-224102.22|共22页
  • 作者单位

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Health, Safety, Radiation Protection Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Nuclear Materials Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Nuclear Materials Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Departamento de Fisica para Ingenieros, Universidad Marista de Merida, Merida, Yucatan 97300, Mexico;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Departamento de Fisica Aplicada Ⅰ, E.T.S. Ingenieria de Bilbao, Universidad del Pais Vasco, Alda. Urquijo s, 48013 Bilbao, Spain;

    Environmental Molecular Sciences Laboratory, Pacific Northwest National Laboratory, Richland, Washington 99352, USA;

    Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Nuclear Materials Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Nuclear Materials Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

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  • 正文语种 eng
  • 中图分类
  • 关键词

    alloys;

    机译:合金;

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