用多量子核磁共振光谱测量溶液中四极核的偶极相互作用

Uzi Eliav, Gil Navon
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引用次数: 9

摘要

偶极相互作用调制引起的弛豫通常用于估计溶液中分子的距离。然而,对于大多数自旋为12的原子核,偶极相互作用引起的单量子跃迁弛豫被四极弛豫所掩盖。本研究表明,即使在单量子弛豫时间由四极相互作用主导的系统中,偶极弛豫也可以通过遵循- m[公式]跃迁来测量。这在溶解于甘油中的配合物[Li-Kryptofix 211]+X−(X = Cl, Br)中的7li中得到了证明,在缓慢运动的温度下,可以观察到noh - 7li NOE。对评价7li的偶极相互作用最重要的弛豫时间是- 12[公式]12和-[公式][公式][公式][公式],它们是通过多量子过滤技术测量的。为了估计四极相互作用,测量了种群的弛豫时间和跃迁的弛豫时间±12[公式]±[公式]。还测量了6li的纵向和横向弛豫时间以及1h - 6li NOE,并与7li测量一起用于获得偶极(D)和四极(χ)相互作用的强度。用几种模型对实验数据进行了分析。给出最佳拟合并产生具有物理意义的参数的模型包括全身各向同性运动以及内部各向异性运动。对于这个特殊的模型,得到了四极和偶极相互作用强度的以下值:D(7Li)/2π = 6.8 kHz, χ(7Li)/2π = 85 kHz和D(6Li)/2π = 1.4 kHz, χ(6Li)/2π = 2.6 kHz。根据ofD的值,计算出锂质子平均距离的估计为3.3 Å,这与晶体学研究相当一致。四极性和偶极相互作用的大小由用于溶液研究的配合物的7li NMR粉末光谱独立确认。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Measurement of Dipolar Interaction of Quadrupolar Nuclei in Solution Using Multiple-Quantum NMR Spectroscopy

Relaxation resulting from the modulation of dipolar interaction is commonly used for estimating distances in molecules in solutions. However, for most nuclei with spinI>12 the single-quantum-transition relaxation by dipolar interaction is masked by quadrupolar relaxation. In the present study, it is shown that even in systems where single-quantum relaxation times are dominated by quadrupolar interaction, dipolar relaxation can be measured by following the −m[formula]mtransitions. This is demonstrated for7Li in the complex [Li–Kryptofix 211]+X(X = Cl, Br) dissolved in glycerol at temperatures for which slow motion prevails and no1H–7Li NOE can be observed. The relaxation times that are most important for the assessment of the dipolar interaction of7Li are −12[formula]12 and −[formula][formula][formula]and they are measured by multiple-quantum-filtration techniques. For estimating the quadrupolar interaction, the relaxation times of the populations and those of the transitions ±12[formula]±[formula]were measured. The longitudinal and transverse relaxation times of6Li as well as the1H–6Li NOE were also measured and, together with the7Li measurements, were used to obtain the strengths of dipolar (D) and quadrupolar (χ) interactions. The experimental data were analyzed using several models to describe the motion. The model that gave the best fit and resulted in parameters that were physically meaningful encompassed a whole-body isotropic motion as well as internal anisotropic motion. For this particular model, the following values for the quadrupolar and the dipolar interactions strength were obtained:D(7Li)/2π = 6.8 kHz, χ(7Li)/2π = 85 kHz andD(6Li)/2π = 1.4 kHz, χ(6Li)/2π = 2.6 kHz. From the value ofD, an estimate of the average lithium–proton distance was calculated to be 3.3 Å, which is in fair agreement with crystallographic studies. The sizes of the quadrupolar and dipolar interactions were independently confirmed by the7Li NMR powder spectra of the complexes that were used for the solution studies.

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