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Lanthanide Ionization Energies and the Sub-Shell Break. Part 1. The Second Ionization Energies

机译:镧系元素电离能量和亚壳断裂。 第1部分。第二电离能量

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By interpolating a 4f(q)6s -> 4f(q)7s transition within the sequence f(1) -> f(14) rather than between f(0) and f(14), revised second ionization energies of the lanthanides have been obtained. In the early part of the series, between cerium and samarium, the revisions are significantly higher than currently accepted values. The revised values have been used to calculate the energy variation for the conversion of Ln(g, 4f(q)6s(2)) to Ln(2+) (g, 4f(q)) across the series Ba -> Yb. The variation is smooth between lanthanum and ytterbium but the barium point at q 5 0 is displaced downwards by more than 0.3 eV, thereby representing a significant sub-shell break. A case is also made for a substantial change to the second ionization energy of lutetium, the revised value being 14.13 +/- 0.10 eV. (C) 2017 AIP Publishing LLC for the National Institute of Standards and Technology.
机译:通过在序列F(1) - > f(14)内的转换而不是在F(0)和F(14)之间,通过内插4F(Q)6S - > 4F(Q)7S转换,镧系元素的修正二次电离能量 获得。 在该系列的早期部分,铈和钐之间,修订显着高于当前接受的值。 经修订的值已被用于计算跨系列BA-> Yb的LN(G,4 +)(G,4F(Q))的LN(G,4F(Q)6s(2))的能量变化。 在镧和镱之间的变化是光滑的,但Q 5 0的钡点向下移动超过0.3eV,从而表示显着的子壳断裂。 还对卢提提的第二电离能量进行了大量变化,修正值为14.13 +/- 0.10eV。 (c)2017年AIP出版LLC为国家标准与技术研究所。

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