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首页> 外文期刊>Russian Journal of Inorganic Chemistry >Theoretical Study of Dodecahydro-closo-Decaborane B_(10)H_(12) the Diprotonated Boron Cluster B_(10)H_(10)~(2-)
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Theoretical Study of Dodecahydro-closo-Decaborane B_(10)H_(12) the Diprotonated Boron Cluster B_(10)H_(10)~(2-)

机译:十二氢-闭-十硼烷B_(10)H_(12)双质子化硼簇B_(10)H_(10)〜(2-)的理论研究

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摘要

The electronic and geometric structures of different isomers of the closo-B_(10)H_(12) boron cluster have been calculated by the density functional theory method (in the B3LYP/6-311 ++G**//B3LYP/6-31G * approximation). The compound is considered to be the diprotonated (H*) analogue of the well-studied B_(10)H_(10)~(2-) anion and serves as a model system. The increase in the relative energies of isomers and the preferred location of the extra H* protons near the opposite B( 1) and B( 10) "poles" are consistent with the charge separation (in the framework of the Mulliken population analysis) between B(l) and B(10). The reactions of migration of one or simultaneously two H* protons in B_(10)H_(12) over the boron polyhedron have been considered, and the corresponding energies of elementary events E and activation barriers h have been estimated. The elementary events have been predicted in which both H* protons simultaneously move along the trajectories near the opposite B(l) and B(10) poles of the B_(10)H_(10)~(2-) polyhedron with the same or opposite changes in the angles determining the H* position with respect to the B(l)-B(10) axis. The activation barrier to the "opposite" migration of the H* protons has been assessed to be h ~ 1.2 kcal/mol, whereas for the migration of the H* protons in the same direction, h~A kcal/mol. The H* proton transfer from the position near the B(l) pole to the position near the opposite B(10) pole is hindered, and higher activation barriers on the order of h ~ 13-15 kcal/mol should be overcome for this transfer to occur.
机译:Closo-B_(10)H_(12)硼团簇的不同异构体的电子和几何结构已通过密度泛函理论方法(在B3LYP / 6-311 ++ G ** // B3LYP / 6- 31G *近似值)。该化合物被认为是经过深入研究的B_(10)H_(10)〜(2-)阴离子的双质子化(H *)类似物,可作为模型系统。异构体的相对能量的增加以及额外的H *质子在相反的B(1)和B(10)“极”附近的优选位置与电荷分离(在Mulliken总体分析的框架内)一致B(1)和B(10)。已经考虑了硼多面体中B_(10)H_(12)中一个或同时两个H *质子迁移的反应,并估计了基本事件E和活化势垒h的相应能量。已经预测了基本事件,其中两个H *质子同时沿着B_(10)H_(10)〜(2-)多面体的相对B(1)和B(10)极在相反的轨迹附近移动,且具有相同或确定相对于B(l)-B(10)轴的H *位置的角度的相反变化。 H *质子“相反”迁移的活化势垒估计为h〜1.2 kcal / mol,而H *质子沿相同方向的迁移则为h〜A kcal / mol。 H *质子从B(l)极附近的位置转移到相对的B(10)极附近的位置受到阻碍,为此,应克服大约h〜13-15 kcal / mol的更高的活化势垒转移发生。

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