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在从头算极限下表征的高度非谐BH5势能面。

The highly anharmonic BH5 potential energy surface characterized in the ab initio limit.

作者信息

Schuurman Michael S, Allen Wesley D, Schleyer Paul von Ragué, Schaefer Henry F

机构信息

Center for Computational Chemistry, University of Georgia, Athens, GA 30602-2525, USA.

出版信息

J Chem Phys. 2005 Mar 8;122(10):104302. doi: 10.1063/1.1853377.

Abstract

The strong sensitivity to level of theory of the salient features of the ground state potential energy surface of BH(5) has been overcome by rigorously converged ab initio computations employing correlation-consistent basis sets cc-p(C)VXZ (X=2-6), explicitly correlated R12 corrections, and coupled-cluster theory complete through quadruple excitations (CCSDTQ). Extrapolations via our focal point method yield a C(s)-symmetry global minimum of BH(3)-H(2) type featuring interfragment B-H distances of (1.401, 1.414) A, an H(2) bond length elongated to 0.803 A, and a BH(3)+H(2) dissociation energy D(e)(D(0))=6.6 (1.2) kcal mol(-1). The classical barriers for H(2) internal rotation and hydrogen scrambling are 0.07 and 5.81 kcal mol(-1), respectively, above the BH(5) minimum. Our thermochemical computations yield Delta(f)H(0) ( degrees )[BH(5)(g)]=-111.3+/-0.2 kcal mol(-1)+Delta(f)H(0) ( degrees )[B(g)], which is limited in accuracy only by persistent uncertainties in the enthalpy of formation of gaseous boron. As a first step in investigating the extremely anharmonic 12-dimensional vibrational dynamics of BH(5), a complete quartic force field has been computed at the all-electron cc-pCVQZ CCSD(T) level of theory. Previous matrix isolation infrared assignments of the nu(2) and nu(9) stretching modes of BH(5) compare favorably with our computed vibrational fundamentals, but the experimental assignment of the nu(6) bending mode of the BH(3) moiety is not supported by computed isotopic shifts.

摘要

通过使用相关一致基组cc-p(C)VXZ(X = 2 - 6)、显式相关的R12校正以及包含四重激发的耦合簇理论(CCSDTQ)进行严格收敛的从头计算,克服了BH(5)基态势能面显著特征对理论水平的强烈敏感性。通过我们的焦点方法外推得到一个具有C(s)对称性的全局最小值,其为BH(3)-H(2)类型,片段间B - H距离为(1.401, 1.414) Å,H(2)键长拉长至0.803 Å,BH(3)+H(2)离解能D(e)(D(0)) = 6.6 (1.2) kcal mol⁻¹。H(2)内旋转和氢重排的经典势垒分别比BH(5)最小值高0.07和5.81 kcal mol⁻¹。我们的热化学计算得出ΔfH(0) (°)[BH(5)(g)] = -111.3 ± 0.2 kcal mol⁻¹ + ΔfH(0) (°)[B(g)],其精度仅受气态硼生成焓持续存在的不确定性限制。作为研究BH(5)极其非谐的12维振动动力学的第一步,已在全电子cc-pCVQZ CCSD(T)理论水平上计算了完整的四次力场。先前对BH(5)的ν₂和ν₉伸缩模式的矩阵隔离红外归属与我们计算的振动基频吻合良好,但BH(3)部分的ν₆弯曲模式的实验归属未得到计算同位素位移的支持。

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