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Theory for α- and δ-Pu

机译:α-和δ-Pu理论

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摘要

During the last few years, there has been intense research, both theoretically and experimentally aimed to understand the fundamental properties of Pu and the anomalous, but technologically important, δ phase. Pu undergoes several phase transitions as a function of temperature at ambient pressure, and δ-Pu, stable between about 600 K and 740 K, is the least dense phase. This phase is quite different from the ground-state α phase, for instance: (ⅰ) δ-Pu has an atomic volume about 25% greater than α-Pu. (ⅱ) The crystal symmetry of δ-Pu is cubic, but α-Pu condenses in a very complex low-symmetry monoclinic phase, (ⅲ) The thermal expansion of δ-Pu is small and negative, but it is very large and positive for α-Pu. These remarkable inconsistencies occur for two phases of Pu separated by only a few hundred degrees and naturally suggest that the electronic structure in Pu is rapidly changing with temperature. The ambient pressure phase diagram of Pu is shown in Figure 1.
机译:在过去的几年中,进行了深入的研究,无论是从理论上还是从实验上,目的都是为了理解Pu的基本性质以及异常的,但在技术上很重要的δ相。 Pu在环境压力下经历数个相变,随温度的变化而变化,δ-Pu稳定在最小600 K和740 K之间,是密度最小的相。该相与基态α相完全不同,例如:(ⅰ)δ-Pu的原子量比α-Pu大25%。 (ⅱ)δ-Pu的晶体对称性是立方的,但α-Pu凝结在一个非常复杂的低对称性单斜晶相中,(ⅲ)δ-Pu的热膨胀小且为负,但非常大且为正对于α-Pu。这些显着的不一致发生在仅相隔几百度的Pu的两个相中,自然地表明Pu的电子结构随温度快速变化。 Pu的环境压力相图如图1所示。

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