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首页> 外文期刊>Chemical science >Magnetic anisotropy of endohedral lanthanide ions: paramagnetic NMR study of MSc2N@C-80-I-h with M running through the whole 4f row
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Magnetic anisotropy of endohedral lanthanide ions: paramagnetic NMR study of MSc2N@C-80-I-h with M running through the whole 4f row

机译:内膜镧系离子的磁各向异性:MSc2N @ C-80-I-h的顺磁NMR研究,M贯穿整个4f行

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Paramagnetic and variable temperature C-13 and Sc-45 nuclear magnetic resonance studies are performed for nitride clusterfullerenes MSc2N@C-80 with icosahedral Ih(7) carbon cage, where M runs through all lanthanides forming nitride clusters. The influence of the endohedral lanthanide ions on the NMR spectral pattern is carefully followed, and dramatic differences are found in peak positions and line widths. Thus, C-13 lines broaden from 0.01-0.02 ppm in diamagnetic MSc2N@C-80 molecules (M = La, Y, Lu) to several ppm in TbSc2N@C-80 and DySc2N@C-80. Direction of the paramagnetic shift depends on the shape of the 4f electron density in corresponding lanthanide ions. In TmSc2N@C-80 and ErSc2N@C-80 with prolate 4f-density of lanthanide ions, C-13 signals are shifted down-field, whereas Sc-45 peaks are shifted up-field versus diamagnetic values. In all other MSc2N@C-80 molecules lanthanide ions have oblate-shaped 4f electron density, and the lanthanide-induced shift is negative for C-13 and positive for Sc-45 peaks. Analysis of the pseudocontact and contact contributions to chemical shifts revealed that the pseudocontact term dominates both in C-13 and Sc-45 NMR spectra, although contact shifts for C-13 signals are also considerable. Point charge computations of the ligand field splitting are performed to explain experimental results, and showed reasonable agreement with experimental pseudocontact shifts. Nitrogen atom bearing large negative charge and located close to the lanthanide ion results in large magnetic anisotropy of lanthanide ions in nitride clusterfullerenes with quasi-uniaxial ligand field.
机译:对具有二十面体Ih(7)碳笼的氮化物簇富勒烯MSc2N @ C-80进行了顺磁和可变温度C-13和Sc-45核磁共振研究,其中M穿过所有镧系元素形成氮化物簇。仔细观察内表面镧系离子对NMR谱图的影响,发现峰位和线宽存在显着差异。因此,C-13谱线从抗磁性MSc2N @ C-80分子(M = La,Y,Lu)中的0.01-0.02 ppm扩大到TbSc2N @ C-80和DySc2N @ C-80中的ppm。顺磁位移的方向取决于相应镧系离子中4f电子密度的形状。在具有4f密度的镧系元素离子的TmSc2N @ C-80和ErSc2N @ C-80中,C-13信号向下磁场偏移,而Sc-45峰向上磁场偏移而与抗磁值相对。在所有其他MSc2N @ C-80分子中,镧系元素离子具有扁圆形的4f电子密度,镧系元素引起的位移对C-13为负,对Sc-45峰为正。分析伪接触和接触对化学位移的贡献后发现,尽管C-13信号的接触位移也很可观,但伪接触项在C-13和Sc-45 NMR光谱中均占主导地位。进行配体场分裂的点电荷计算以解释实验结果,并显示出与实验伪接触位移合理的一致性。带有大负电荷且靠近镧系元素离子的氮原子会导致氮化物簇富勒烯中具有准单轴配体场的镧系元素离子具有较大的磁各向异性。

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