首页> 外文OA文献 >A systematic comparison of second-order polarization propagator approximation (SOPPA) and equation-of-motion coupled cluster singles and doubles (EOM#CCSD) spin#spin coupling constants for selected singly bonded molecules, and the hydrides NH, HO, and HF and their protonated and deprotonated ions and hydrogen-bonded complexes
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A systematic comparison of second-order polarization propagator approximation (SOPPA) and equation-of-motion coupled cluster singles and doubles (EOM#CCSD) spin#spin coupling constants for selected singly bonded molecules, and the hydrides NH, HO, and HF and their protonated and deprotonated ions and hydrogen-bonded complexes

机译:对选定单键分子和氢化物NH,HO和HF的二阶极化传播器近似(SOPPA)和运动方程耦合簇单双态(EOM#CCSD)自旋#spin耦合常数的系统比较它们的质子化和去质子化离子以及氢键络合物

摘要

Second-order polarization propagator approximation (SOPPA) and equation-of-motion coupled cluster singles and doubles (EOM-CCSD) methods have been employed for the calculation of one-bond spin-spin coupling constants in series of small molecules and ions, and of one- and two-bond coupling constants across X-H⋯Y hydrogen bonds. For isolated molecules, one-bond SOPPA coupling constants 1J(X-Y) involving 13C, 15N, 17O, and 19F have larger absolute values than corresponding EOM-CCSD coupling constants, with the EOM-CCSD values being in significantly better agreement with available experimental data. The difference between SOPPA and EOM-CCSD tends to increase as the number of nonbonding electrons on the coupled atoms increases, and the SOPPA values for O-F coupling are significantly in error. Similarly, the absolute values of SOPPA one-bond coupling constants 1J(X-H) for the hydrides NH3, H 2O, and FH and their protonated and deprotonated ions are greater than EOM-CCSD values, with the largest differences occurring for F-H coupling. One- and two-bond coupling constants 1J(X-H), 1hJ(H-Y), and 2hJ(X-Y) across X-H⋯;Y hydrogen bonds in neutral, protonated, and deprotonated complexes formed from the hydrides are similar at SOPPA and EOM-CCSD, with the largest differences again found for 1J(F-H) in complexes with F-H as the proton donor, and 2hJ(F-F) for (FHF)-. The signs of 1J(X-H), 1hV(H-Y), and 2hJ(X-Y) are the same at both levels of theory, as is their variation across the proton-transfer coordinate in F-H⋯;NH3. SOPPA would appear to provide a reliable and more cost-effective alternative approach for computing coupling constants across hydrogen bonds, although couplings involving F may be problematic. © 2008 American Chemical Society.
机译:二阶极化传播器近似(SOPPA)和运动方程耦合簇单双态(EOM-CCSD)方法已用于计算一系列小分子和离子中的单键自旋自旋耦合常数,并且XH⋯Y氢键的一键和双键耦合常数对于分离的分子,涉及13C,15N,17O和19F的单键SOPPA耦合常数1J(XY)的绝对值大于相应的EOM-CCSD耦合常数,并且EOM-CCSD值与可用的实验数据明显更好地吻合。随着耦合原子上非键电子数量的增加,SOPPA与EOM-CCSD之间的差异趋于增加,并且O-F耦合的SOPPA值存在明显误差。同样,氢化物NH3,H 2O和FH及其质子化和去质子化离子的SOPPA单键耦合常数1J(X-H)的绝对值大于EOM-CCSD值,其中F-H耦合的差异最大。跨越XH⋯的一键和双键耦合常数1J(XH),1hJ(HY)和2hJ(XY);由氢化物形成的中性,质子化和去质子化的配合物中的Y氢键在SOPPA和EOM-CCSD上相似,在以FH为质子供体的复合物中1J(FH)和(FHF)-的2hJ(FF)的差异再次最大。 1J(X-H),1hV(H-Y)和2hJ(X-Y)的符号在两个理论水平上都是相同的,它们在F-H⋯; NH3中跨质子传递坐标的变化也是如此。尽管涉及F的偶联可能存在问题,但SOPPA似乎为计算跨氢键的偶联常数提供了一种可靠且更具成本效益的替代方法。 ©2008美国化学学会。

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