Skip to main content
. 2022 Apr 28;126(18):2802–2810. doi: 10.1021/acs.jpca.2c01376

Table 1. Energies (kcal/mol) at Different Levels of Theory and Their Auxiliary Corrections (kcal/mol) for the Stationary Points and Product Channels of the Cl(2P3/2) + CH3CN Reaction Relative to the Reactants.

  MP2 CCSD(T)-F12b
               
stationary points aVDZa aVDZb aVTZc aVQZd δ[T]e δ[(Q)]f Δcoreg Δrelh ΔSOi classicalj ΔZPEk adiabaticl
H Abs TS 7.28 7.43 7.98 7.93 –0.36 –0.26 –0.04 +0.07 +0.80 8.15 –4.39 3.76
CH3 Sub C-side TS 33.90 29.78 31.09 31.08 –0.64 –0.36 +0.28 +0.18 +0.83 31.36 –2.38 28.98
H Sub W TS 51.62 49.71 50.31 50.27 –0.23 –0.43 +0.21 +0.05 +0.81 50.69 –4.07 46.62
CN Sub W TS 57.51 54.73 54.82 54.83 –1.32 –0.67 +0.65 +0.01 +0.78 54.27 –1.73 52.54
CH3 Sub N-side TS 64.25 60.28 60.90 61.02 –0.13 –0.09 +0.77 –0.11 +0.68 62.15 –1.58 60.57
H Sub FS TS 67.41 65.12 65.93 65.92 –0.39 –0.48 +0.18 +0.00 +0.83 66.05 –4.25 61.80
CN Sub FS TS 77.14 74.40 75.05 75.07 –1.49 –0.86 +0.64 –0.10 +0.81 74.08 –1.63 72.45
H Abs MIN –6.95 –9.26 –8.33 –8.43 –0.45 –0.09 –0.07 +0.27 +0.83 –7.94 –3.50 –11.44
CH3 Sub C-side MIN 25.53 20.72 22.29 22.25 +0.02 –0.23 +0.12 +0.20 +0.83 23.19 –3.90 19.28
H Sub W MIN 26.00 27.29 28.83 28.80 +0.15 –0.23 +0.04 +0.18 +0.83 29.77 –4.83 24.95
CH3 Sub N-side MIN 75.18 64.14 65.81 65.87 –0.15 –0.05 +0.51 +0.16 +0.83 67.17 –4.55 62.62
H Sub FS MIN 25.98 27.11 28.76 28.73 +0.15 –0.23 +0.04 +0.18 +0.83 29.70 –4.79 24.91
CN Sub FS MIN 38.82 34.44 35.21 35.22 –1.17 –0.45 +0.52 +0.11 +0.83 35.06 –0.71 34.35
HCl + CH2CN –0.78 –3.82 –3.11 –3.21 –0.48 –0.06 +0.00 +0.23 +0.83 –2.68 –4.74 –7.42
ClCN + CH3 27.06 22.05 23.55 23.48 +0.02 –0.22 +0.13 +0.20 +0.83 24.43 –4.30 20.13
ClCH2CN + H 26.30 27.65 29.19 29.14 +0.15 –0.22 +0.04 +0.18 +0.83 30.12 –5.18 24.94
ClNC + CH3 76.55 65.41 66.89 66.91 –0.16 –0.03 +0.52 +0.17 +0.83 68.25 –4.94 63.31
CH3Cl + CN 44.32 38.94 39.51 39.44 –1.59 –0.48 +0.60 +0.15 +0.83 38.96 –1.60 37.36
a

MP2/aug-cc-pVDZ relative energies obtained at MP2/aug-cc-pVDZ geometries.

b

CCSD(T)-F12b/aug-cc-pVDZ relative energies obtained at CCSD(T)-F12b/aug-cc-pVDZ geometries.

c

CCSD(T)-F12b/aug-cc-pVTZ relative energies obtained at CCSD(T)-F12b/aug-cc-pVTZ geometries.

d

CCSD(T)-F12b/aug-cc-pVQZ relative energies obtained at CCSD(T)-F12b/aug-cc-pVTZ geometries.

e

CCSDT – CCSD(T) obtained at CCSD(T)-F12b/aug-cc-pVTZ geometries with the aug-cc-pVDZ basis set.

f

CCSDT(Q) – CCSDT obtained at CCSD(T)-F12b/aug-cc-pVTZ geometries with the aug-cc-pVDZ basis set.

g

Core correlation corrections obtained as the differences between all-electron and frozen-core CCSD(T)-F12b/cc-pCVTZ-F12 relative energies at CCSD(T)-F12b/aug-cc-pVTZ geometries.

h

Scalar relativistic effects obtained as the difference between DK-AE-CCSD(T)/aug-cc-pwCVTZ-DK and AE-CCSD(T)/aug-cc-pwCVTZ relative energies at CCSD(T)-F12b/aug-cc-pVTZ geometries.

i

Spin–orbit (SO) corrections obtained as the differences between the SO and non-SO ground-state MRCI+Q/aug-cc-pwCVTZ relative energies at CCSD(T)-F12b/aug-cc-pVTZ geometries.

j

Benchmark classical relative energies obtained as CCSD(T)-F12b/aug-cc-pVQZ relative energies + δ[T] (e) + δ[(Q)] (f) + Δcore (g) + Δrel (h) + ΔSO (i).

k

Zero-point energy (ZPE) corrections obtained at CCSD(T)-F12b/aug-cc-pVTZ.

l

Benchmark vibrationally adiabatic relative energies obtained as classical relative energies (j) + ΔZPE (k).