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Estimated MP2 and CCSD(T) interaction energies of n-alkane dimers at the basis set limit: Comparison of the methods of Helgaker et al. and Feller

机译:正基烷二聚体估计的MP2和CCSD(T)相互作用能在基集极限下:Helgaker等人方法的比较。和费勒

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The MP2 (the second-order Moller-Plesset calculation) and CCSD(T) (coupled cluster calculation with single and double substitutions with noniterative triple excitations) interaction energies of all-trans n-alkane dimers were calculated using Dunning's [J. Chem. Phys. 90, 1007 (1989)] correlation consistent basis sets. The estimated MP2 interaction energies of methane, ethane, and propane dimers at the basis set limit [E-MP2(limit)] by the method of Helgaker [J. Chem. Phys. 106, 9639 (1997)] from the MP2/aug-cc-pVXZ (X=D and T) level interaction energies are very close to those estimated from the MP2/aug-cc-pVXZ (X=T and Q) level interaction energies. The estimated E-MP2(limit) values of n-butane to n-heptane dimers from the MP2/cc-pVXZ (X=D and T) level interaction energies are very close to those from the MP2/aug-cc-pVXZ (X=D and T) ones. The E-MP2(limit) values estimated by Feller's [J. Chem. Phys. 96, 6104 (1992)] method from the MP2/cc-pVXZ (X=D, T, and Q) level interaction energies are close to those estimated by the method of Helgaker from the MP2/cc-pVXZ (X=T and Q) ones. The estimated E-MP2(limit) values by the method of Helgaker using the aug-cc-pVXZ (X=D and T) are close to these values. The estimated E-MP2(limit) of the methane, ethane, propane, n-butane, n-pentane, n-hexane, n-heptane, n-octane, n-nonane, and n-decane dimers by the method of Helgaker are -0.48, -1.35, -2.08, -2.97, -3.92, -4.91, -5.96, -6.68, -7.75, and -8.75 kcal/mol, respectively. Effects of electron correlation beyond MP2 are not large. The estimated CCSD(T) interaction energies of the methane, ethane, propane, and n-butane dimers at the basis set limit by the method of Helgaker (-0.41, -1.22, -1.87, and -2.74 kcal/mol, respectively) from the CCSD(T)/cc-pVXZ (X=D and T) level interaction energies are close to the E-MP2(limit) obtained using the same basis sets. The estimated E-MP2(limit) values of the ten dimers were fitted to the form m(0)+m(1)X (X is 1 for methane, 2 for ethane, etc.). The obtained m(0) and m(1) (0.595 and -0.926 kcal/mol) show that the interactions between long n-alkane chains are significant. Analysis of basis set effects shows that cc-pVXZ (X=T, Q, or 5), aug-cc-pVXZ (X=D, T, Q, or 5) basis set, or 6-311G(**) basis set augmented with diffuse polarization function is necessary for quantitative evaluation of the interaction energies between n-alkane chains. (c) 2006 American Institute of Physics.
机译:使用邓宁的方法计算全反式正构烷烃二聚体的MP2(二阶Moller-Plesset计算)和CCSD(T)(具有非迭代三重激发的单取代和双取代的耦合簇计算)[J]。化学物理90,1007(1989)]相关一致的基集。甲烷,乙烷和丙烷二聚体的MP2相互作用能通过Helgaker方法估计在基本设定的极限值[E-MP2(limit)]。化学物理106,9639(1997)]从MP2 / aug-cc-pVXZ(X = D和T)级相互作用能中得出的能量非常接近从MP2 / aug-cc-pVXZ(X = T和Q)级相互作用所估计出的能量。能量。从MP2 / cc-pVXZ(X = D和T)级相互作用能估计的正丁烷至正庚烷二聚体的E-MP2(极限)值非常接近MP2 / aug-cc-pVXZ( X = D和T)个。 E-MP2(极限)值由Feller [J.化学物理96,6104(1992)]从MP2 / cc-pVXZ(X = D,T和Q)级的相互作用能中获得的能量与通过Helgaker方法从MP2 / cc-pVXZ(X = T和T问)。通过Helgaker方法使用aug-cc-pVXZ估算的E-MP2(极限)值(X = D和T)接近于这些值。通过Helgaker方法估算的甲烷,乙烷,丙烷,正丁烷,正戊烷,正己烷,正庚烷,正辛烷,正壬烷和正癸烷二聚物的E-MP2(极限)分别为-0.48,-1.35,-2.08,-2.97,-3.92,-4.91,-5.96,-6.68,-7.75和-8.75 kcal / mol。超出MP2的电子相关性影响不大。通过Helgaker方法估算的甲烷,乙烷,丙烷和正丁烷二聚体的CCSD(T)相互作用能在基准设置极限处分别为-0.41,-1.22,-1.87和-2.74 kcal / mol。来自CCSD(T)/ cc-pVXZ(X = D和T)级的相互作用能接近使用相同基集获得的E-MP2(极限)。将十个二聚体的估计E-MP2(极限)值拟合为m(0)+ m(1)X的形式(X对于甲烷为1,对于乙烷为2,等等)。获得的m(0)和m(1)(0.595和-0.926 kcal / mol)表明长正构烷烃链之间的相互作用非常显着。基集效应分析显示,使用cc-pVXZ(X = T,Q或5),aug-cc-pVXZ(X = D,T,Q或5)基集或6-311G(**)基为了定量评估正构烷烃链之间的相互作用能,有必要增加扩散极化函数集。 (c)2006年美国物理研究所。

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