LLNLがプルトニウムの特異な挙動を説明する新しいモデルを実証(LLNL demonstrates new model that explains plutonium’s peculiar behavior)

2025-08-06 ローレンスリバモア国立研究所(LLNL)

米ローレンス・リバモア国立研究所(LLNL)の研究チームは、プルトニウムの異常な熱的挙動、特にδ相で加熱時に収縮する現象を説明する新モデルを開発した。自由エネルギー計算に温度依存の磁気ゆらぎを導入することで、従来の理論では説明できなかった実験結果と整合性を持たせることに成功。このアプローチは鉄など他の動的磁性材料にも応用可能であり、今後は微細構造や欠陥の影響にも研究を拡大予定。核材料の理解と設計に新たな道を拓く成果である。

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δ-プルトニウムの動的磁性を考慮した第一原理自由エネルギーモデル First principles free energy model with dynamic magnetism for δ-plutonium

Per Söderlind, A Landa, L X Benedict, N Goldman, R Q Hood, K E Kweon, E E Moore, A Perron, B Sadigh, C J Wu,…
Reports on Progress in Physics  Published: 21 July 2025
DOI:10.1088/1361-6633/adedb1

Abstract

We present an ab initio free energy model derived from a fully relativistic density functional theory (DFT) electronic structure with dynamic magnetism for δ-plutonium (face-centered cubic, fcc). The DFT model is extended with orbital-orbital interaction in a parameter free orbital polarization (OP) mechanism consistent with previous modeling of plutonium. Gibbs free energy is built from components associated with the temperature dependence of the electronic structure and the corresponding electronic entropy, lattice vibrations within an anharmonic lattice dynamics model, and dynamical fluctuations of the magnetization density, i.e. magnetic fluctuations. The fluctuation model consists of transverse and longitudinal modes driven by temperature induced excitations of the DFT + OP electronic structure. The ab initio model thus incorporates fluctuating states beyond the electronic ground state. Thanks to the dynamic magnetism, the theory predicts excellent thermodynamic properties and a Gibbs free energy in accord with CALPHAD and semi-empirical modeling developed from the thermodynamic observables. The magnetic fluctuations further explain anomalous behaviors of the thermal expansion in plutonium. Specifically, a thermal expansion for the δ-plutonium system turning from positive to negative at temperatures above room temperature, a tendency for gallium to reduce and remove the negative thermal expansion depending on composition, and a positive thermal expansion for the high temperature epsilon phase.

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