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Y@C82 金属富勒烯在固体氩基质中的 EPR 光谱:EPR 光谱和相对论 DFT 计算的超精细结构。

EPR spectrum of the Y@C82 metallofullerene isolated in solid argon matrix: hyperfine structure from EPR spectroscopy and relativistic DFT calculations.

机构信息

Institute of Problems of Chemical Physics of the Russian Academy of Sciences, 142432 Chernogolovka, Moscow Region, Russia.

出版信息

Phys Chem Chem Phys. 2010 Aug 21;12(31):8863-9. doi: 10.1039/b926279b. Epub 2010 Jun 9.

DOI:10.1039/b926279b
PMID:20535405
Abstract

The EPR spectrum of the Y@C(82) molecules isolated in solid argon matrix was recorded for the first time at a temperature of 5 K. The isotropic hyperfine coupling constant (hfcc) A(iso) = 0.12 +/- 0.02 mT on the nucleus (89)Y as derived from the EPR spectrum is found in more than two times greater than that obtained in previous EPR measurements in liquid solutions. Comparison of the measured hfcc on a metal atom with that predicted by density-functional theory calculations (PBE/L22) indicate that relativistic method provides good agreement between experiment in solid argon and theory. Analysis of the DFT calculated dipole-dipole hf-interaction tensor and electron spin distribution in the endometallofullerenes with encaged group 3 metal atoms Sc, Y and La has been performed. It shows that spin density on the scandium atom represents the Sc d(yz) orbital lying in the symmetry plane of the C(2v) fullerene isomer and interacting with two carbon atoms located in the para-position on the fullerene hexagon. In contrast, the configuration of electron spin density on the heavier atoms, Y and La, is associated with the hybridized orbital formed by interaction of the metal d(yz) and p(y) electronic orbitals.

摘要

首次在 5 K 的温度下记录了 Y@C(82)分子在固体氩基质中的 EPR 光谱。从 EPR 光谱中得出的核(89)Y 的各向同性超精细耦合常数(hfcc)A(iso) = 0.12 +/- 0.02 mT 比以前在液体溶液中的 EPR 测量值大两倍多。将测量的金属原子上的 hfcc 与密度泛函理论计算(PBE/L22)预测值进行比较表明,相对论方法在固体氩中的实验和理论之间提供了很好的一致性。分析了内包第 3 族金属原子 Sc、Y 和 La 的endo 金属富勒烯中的偶极-偶极 hf 相互作用张量和电子自旋分布。结果表明,位于 C(2v)富勒烯异构体对称面内并与位于富勒烯六边形对位的两个碳原子相互作用的 Sc d(yz)轨道上的自旋密度代表了钪原子上的自旋密度。相比之下,较重原子 Y 和 La 上的电子自旋密度构型与金属 d(yz)和 p(y)电子轨道相互作用形成的杂化轨道有关。

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