Tossell J A, Liu Yun
Department of Chemistry and Biochemistry, University of Maryland, College Park, Maryland 20742, USA.
Magn Reson Chem. 2004 Oct;42 Spec no:S34-40. doi: 10.1002/mrc.1434.
(19)F and (27)Al NMR chemical shifts are calculated for the F and Al atoms of the mineral rosenbergite, AlFF(0.5)(H(2)O)(0.5).H(2)O The structure of rosenbergite consists of infinite chains of F-corner-sharing Al[F(4)(H(2)O)(2)] octahedra and isolated water molecules. An F-centered molecular cluster of composition Al(2)F(3)(OH(2))(8) (3+) was initially used to model the mineral, with geometries taken both from the two different available x-ray crystal structures and from equilibrium geometries calculated at the 6-31G* B3LYP level (both with and without polarizable continuum solvation). Related Al(F)F(n) em leader clusters, with additional F(-) replacing H(2)O, were also studied. A larger Al-centered cluster model Al(3)F(4)(OH(2))(12) (5+) was also generated from one of the x-ray geometries and produced very similar bridging F shieldings but slightly different Al shieldings. The NMR shieldings were calculated using both HF and B3LYP GIAO methods, with 6-311+G(2df,p) basis sets, and the HF and B3LYP results averaged for the F shieldings as described in previous work. Calculated (19)F NMR shifts (relative to CCl(3)F) using this procedure were within a few ppm of experiment when either set of x-ray crystal structure coordinates was used, but differed by as much as 20 ppm for the energy-optimized geometries. Rosenbergite-like fragments with geometries optimized in water, simulated by a PCM, were used to model Al hydroxyfluoride species in solution. The (19)F NMR shifts for the bridging F atoms in several such model complexes are very similar to those usually attributed to monomeric species such as Al(OH(2))(5)F(2+) in solution, suggesting that the solution species are actually corner bridging oligomers. The F in the monomeric Al(OH(2))(5)F(2+) solution species is too strongly shielded by about 20 ppm to match the experimental peak usually assigned to it.
计算了矿物罗森伯格石(AlF[F(0.5)(H₂O)(0.5)]₄·H₂O)中F和Al原子的¹⁹F和²⁷Al NMR化学位移。罗森伯格石的结构由F角共享的Al[F₄(H₂O)₂]八面体的无限链和孤立的水分子组成。最初使用组成式为Al₂F₃(OH₂)₈(³⁺)的以F为中心的分子簇对该矿物进行建模,其几何结构取自两种不同的可用X射线晶体结构以及在6 - 31G* B3LYP水平(包括有和没有极化连续介质溶剂化的情况)计算得到的平衡几何结构。还研究了相关的Al(F)Fₙ簇,其中额外的F⁻取代了H₂O。还从一种X射线几何结构生成了更大的以Al为中心的簇模型Al₃F₄(OH₂)₁₂(⁵⁺),其产生了非常相似的桥连F屏蔽,但Al屏蔽略有不同。使用HF和B3LYP GIAO方法,以6 - 311 + G(2df,p)基组计算NMR屏蔽,并且如先前工作所述,对F屏蔽的HF和B3LYP结果进行平均。当使用任何一组X射线晶体结构坐标时,使用此程序计算的¹⁹F NMR位移(相对于CCl₃F)与实验值相差在几个ppm以内,但对于能量优化的几何结构,相差多达20 ppm。通过PCM模拟在水中优化几何结构的类罗森伯格石片段,用于模拟溶液中的羟基氟化铝物种。几种此类模型配合物中桥连F原子的¹⁹F NMR位移与通常归因于溶液中单体物种(如Al(OH₂)₅F²⁺)的位移非常相似,这表明溶液物种实际上是角桥连低聚物。单体Al(OH₂)₅F²⁺溶液物种中的F屏蔽太强,大约相差20 ppm,无法与通常分配给它的实验峰匹配。