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Essentials of Computational Chemistry

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286 8 DENSITY FUNCTIONAL THEORY<br />

Table 8.2 Mean absolute errors in metal–ligand binding<br />

energies for different methods (kcal mol −1 ) a<br />

Level <strong>of</strong> theory b Ligand<br />

H CH3 CH2<br />

MO theoretical methods<br />

MCPF 6 9 20<br />

QCISD(T) 6<br />

PCI-80<br />

Density functional methods<br />

2 2 4<br />

SVWN 12<br />

BP86 8<br />

BH&HLYP 16<br />

BH&HLYP/ECP 5 9<br />

B3LYP 5 6 4<br />

B3LYP/ECP 9 7<br />

a Complexes MX + where M = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu,<br />

and X = ligand.<br />

b Basis sets are for the most part double-ζ polarized in quality. Use<br />

<strong>of</strong> metal effective core potentials is indicated by ECP.<br />

that the pure DFT functional BLYP badly underestimated the activation enthalpies for the<br />

H-atom transfer reactions. This behavior has since been noted by many other authors, and<br />

is part <strong>of</strong> the motivation for the MPW1K model discussed in Section 8.4.3.<br />

In a different analysis <strong>of</strong> hydrogen-atom transfer reaction barriers, Lynch and Truhlar<br />

(2003b) considered the forward and reverse barriers for 22 such reactions, and then demonstrated<br />

that the performance <strong>of</strong> various models on only six data (the forward and reverse<br />

barrier heights for HO + CH4 → H2O + CH3, H+ OH → O + H2, andH+ H2S → H2 +<br />

HS) was highly predictive <strong>of</strong> their accuracy for all 44 barrier heights. In this and subsequent<br />

work by Zhao et al. (2004), they assayed the accuracy <strong>of</strong> a substantial number <strong>of</strong> different<br />

models for this test set and found that modern functionals, and particularly those including a<br />

dependence on the kinetic energy density, gave the best results (Table 8.3, Reaction Set 2).<br />

However, all <strong>of</strong> the geometries used in this analysis were obtained at the QCISD/MG3 level<br />

(partly in recognition <strong>of</strong> the multideterminantal character <strong>of</strong> many H-atom transition-state<br />

structures). So, the reported errors might be expected to change somewhat were geometries<br />

to be located at the DFT levels <strong>of</strong> theory. In this regard, it is noteworthy that Kang and<br />

Musgrave (2001) examined 29 different barrier heights for H-atom transfer using geometries<br />

optimized at the same level as used to compute energies, and reported mean unsigned errors<br />

<strong>of</strong> 0.9, 3.3, 3.2, and 2.9 kcal mol −1 , respectively, for KMLYP, B3LYP, BH&HLYP, and G2.<br />

With respect to chemical reactions not involving H-atom transfer, Guner et al. (2003,<br />

2004) examined a set <strong>of</strong> 11 pericyclic organic reactions having experimental data available<br />

for nine enthalpies <strong>of</strong> activation and six enthalpies <strong>of</strong> forward reaction. They found the<br />

B3LYP and MPW1K functionals to be about as accurate for the activation enthalpies as the<br />

more expensive CBS-QB3 and CASPT2 levels, with other functionals doing somewhat less<br />

well (Table 8.3, Reaction Set 3). Interestingly, they found the performance <strong>of</strong> the B3LYP

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