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镎多极矩和二氧化镎(NpO2)的共振 X 射线布拉格衍射。

Neptunium multipoles and resonant x-ray Bragg diffraction by neptunium dioxide (NpO2).

机构信息

ISIS Facility, STFC, Oxfordshire OX11 0QX, UK.

出版信息

J Phys Condens Matter. 2012 Jun 27;24(25):256009. doi: 10.1088/0953-8984/24/25/256009.

DOI:10.1088/0953-8984/24/25/256009
PMID:22652978
Abstract

The low-temperature ordered state of neptunium dioxide (NpO(2)) remains enigmatic. After decades of experimental and theoretical efforts, long-range order of a time-odd (magnetic) high-order atomic multipole moment is now generally considered to be the fundamental order parameter, the most likely candidate being a magnetic triakontadipole (rank 5). To date, however, direct experimental observation of the primary order parameter remains outstanding. In the light of new experimental findings, we re-examine the effect of crystal symmetry on the atomic multipoles and the resulting x-ray resonant scattering signature. Our simulations use the crystallographic point group ̅3m (D(3d)), because corresponding magnetic groups ̅3m', ̅3'm', and ̅3'm are shown by us to be at odds with a wealth of experimental results. In addition to the previously observed (secondary) quadrupole order, we derive expressions for higher-order multipoles that might be observed in future experiments. In particular, magnetic octupole moments are predicted to contribute to Np M(2,3) and L(2,3) resonant scattering via E2–E2 events. The Lorentzian-squared lineshape observed at the M(4) resonance is shown to be the result of the anisotropy of the 3p(3/2) core levels. Quantitative comparison of our calculations to the measured data yields a core–hole width Γ = 2.60(7) eV and a core-state exchange energy [absolute value]ε(1/2)[absolute value] = 0.76(2) eV.

摘要

二氧化二钚(NpO(2))的低温有序态仍然是一个谜。经过几十年的实验和理论努力,现在普遍认为时间奇(磁)高阶原子多极矩的长程有序是基本的有序参数,最有可能的候选者是磁三圆锥偶极矩(阶数 5)。然而,到目前为止,对主要有序参数的直接实验观察仍然是突出的。鉴于新的实验发现,我们重新检查了晶体对称性对原子多极矩的影响,以及由此产生的 X 射线共振散射特征。我们的模拟使用晶体学点群 ̅3m(D(3d)),因为我们表明相应的磁点群 ̅3m'、 ̅3'm' 和 ̅3'm' 与大量实验结果不一致。除了以前观察到的(次要)四极有序外,我们还推导出了在未来实验中可能观察到的更高阶多极矩的表达式。特别是,磁八极矩有望通过 E2–E2 事件对 Np M(2,3) 和 L(2,3) 共振散射做出贡献。在 M(4)共振处观察到的洛伦兹平方线形状被证明是 3p(3/2)芯能级各向异性的结果。我们的计算与测量数据的定量比较得出芯孔宽度 Γ = 2.60(7)eV 和芯态交换能 [绝对值]ε(1/2)[绝对值] = 0.76(2)eV。

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