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测量 [(199)Hg, (31)P] 的 ΔJ((199)Hg, (31)P) 值和汞-磷耦合张量的相对论 ZORA DFT 研究。

Measurement of delta(1)J((199)Hg, (31)P) in [HgPCy3(OAc)2]2 and relativistic ZORA DFT investigations of mercury-phosphorus coupling tensors.

机构信息

Department of Chemistry and Centre for Catalysis Research and Innovation, University of Ottawa, Ottawa, Ontario, Canada K1N6N5.

出版信息

Solid State Nucl Magn Reson. 2009 Dec;36(4):182-91. doi: 10.1016/j.ssnmr.2009.11.004. Epub 2009 Dec 3.

Abstract

Using 31P solid-state NMR spectroscopy, anisotropy in the indirect 199Hg-31P spin-spin coupling tensor (DeltaJ) for powdered [HgPCy3(OAc)2]2 (1) has been measured as 4700 +/- 300 Hz. Zeroth-order regular approximation (ZORA) density functional theory (DFT) calculations, including scalar and spin-orbit relativistic effects, performed on 1 and a series of other related compounds show that DeltaJ(199Hg, (31)P) arises entirely from the ZORA Fermi-contact-spin-dipolar cross term. The calculations validate assumptions made in the spectral analysis of 1 and in previous determinations of DeltaJ in powder samples, namely that J is axially symmetric and shares its principal axis system with the direct dipolar coupling tensor (D). Agreement between experiment and theory for various 199Hg, 31P spin-spin coupling anisotropies is reasonable; however, experimental values of 1J(199Hg, 31P)(iso) are significantly underestimated by the calculations. The most important improvements in the agreement were obtained as a result of including more of the crystal lattice in the model used for the calculations, e.g., a change of 43% was noted for 1J(199Hg, 31P)(iso) in [HgPPh3(NO3)2]2 depending on whether the two or three nearest nitrate ions are included in the model. Finally, we have written a computer program to simulate the effects of non-axial symmetry in J and of non-coincidence of the J and D on powder NMR spectra. Simulations clearly show that both of these effects have a pronounced impact on the 31P NMR spectrum of 199Hg-31P spin pairs, suggesting that the effects should be observable experimentally if a suitable compound can be identified.

摘要

利用 31P 固态 NMR 光谱学,我们测量了粉末状 [HgPCy3(OAc)2]2(1)中间接 199Hg-31P 自旋-自旋耦合张量(DeltaJ)的各向异性,结果为 4700 +/- 300 Hz。零阶正则逼近(ZORA)密度泛函理论(DFT)计算,包括标量和自旋轨道相对论效应,在 1 和一系列其他相关化合物上进行,表明 DeltaJ(199Hg, (31)P)完全来自于 ZORA 费米接触-自旋偶极交叉项。这些计算验证了在 1 的光谱分析和以前在粉末样品中确定 DeltaJ 时所做的假设,即 J 是轴对称的,并与其直接偶极耦合张量(D)共享其主轴系统。各种 199Hg、31P 自旋-自旋耦合各向异性的实验值与理论值之间的一致性是合理的;然而,计算明显低估了 1 的 1J(199Hg, 31P)(iso)值。通过在计算中纳入更多的晶体晶格,从而使计算模型更加准确,从而使一致性得到了最大程度的提高,例如,对于[HgPPh3(NO3)2]2 中的 1J(199Hg, 31P)(iso),如果模型中包含两个或三个最近的硝酸盐离子,其变化分别为 43%。最后,我们编写了一个计算机程序来模拟 J 的非轴对称性和 J 与 D 的非重合性对粉末 NMR 光谱的影响。模拟清楚地表明,这两种效应都会对 199Hg-31P 自旋对的 31P NMR 谱产生显著影响,这表明如果能识别出合适的化合物,这些效应在实验中应该是可以观察到的。

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