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Essentials of Computational Chemistry

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8.6 GENERAL PERFORMANCE OVERVIEW OF DFT 285<br />

spin-orbit corrections and updated experimental data for the heats <strong>of</strong> formation <strong>of</strong> the silicon<br />

and beryllium atoms and carbonyl difluoride, while others do not. Readers may refer to the<br />

original literature listed in the bibliography for full details.<br />

Some key points may be inferred from Table 8.1.<br />

1. For a given average level <strong>of</strong> accuracy, hybrid and meta-GGA DFT methods are obviously<br />

the most efficient, showing mean unsigned errors almost equal in quality to the much<br />

more expensive multilevel correlated methods. However, the maximum absolute errors<br />

are larger with the former methods than the latter, indicating a slightly lower generality<br />

even in the most current generation <strong>of</strong> functionals.<br />

2. Hybrid and meta-GGA DFT functionals usually <strong>of</strong>fer some improvement over corresponding<br />

pure DFT functionals.<br />

3. Increasing basis-set size does not always improve the accuracy <strong>of</strong> the DFT models,<br />

although it must, <strong>of</strong> course, ultimately lead to a converged prediction.<br />

4. Of the currently available DFT models, it is clear that GGA models <strong>of</strong>fer a major<br />

improvement over the older LSDA model. It further appears that the P86 functional<br />

should be avoided. With respect to a more specific ranking <strong>of</strong> functionals, Boese, Martin<br />

and Handy (2003) have carried out a careful evaluation <strong>of</strong> a large number <strong>of</strong> functionals<br />

for various energetic quantities (atomization enthalpies, IPs, EAs, geometries, etc.) using<br />

polarized triple-ζ basis sets. They conclude that for pure GGA functionals an error<br />

ranking (i.e., lower is better) is HCTH < OLYP < BPW91 < BLYP

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