Spin-State Corrected Gaussian-Type Orbital Basis Sets
Recently, we reported that the basis set has a profound influence on the computed values for spin-state splittings [J. Phys. Chem. A 2008, 112, 6384]. In particular, small Gaussian-type orbital basis sets were shown to be unreliable for the prediction of them. Here, we report simple modifications of...
| Autores: | , , , |
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| Tipo de recurso: | artículo |
| Estado: | Versión aceptada para publicación |
| Fecha de publicación: | 2010 |
| País: | España |
| Institución: | Varias* (Consorci de Biblioteques Universitáries de Catalunya, Centre de Serveis Científics i Acadèmics de Catalunya) |
| Repositorio: | Recercat. Dipósit de la Recerca de Catalunya |
| OAI Identifier: | oai:recercat.cat:10256/16587 |
| Acceso en línea: | http://hdl.handle.net/10256/16587 |
| Access Level: | acceso abierto |
| Palabra clave: | Polarització (Física nuclear) Polarization (Nuclear physics) Orbitals moleculars Molecular orbitals |
| Sumario: | Recently, we reported that the basis set has a profound influence on the computed values for spin-state splittings [J. Phys. Chem. A 2008, 112, 6384]. In particular, small Gaussian-type orbital basis sets were shown to be unreliable for the prediction of them. Here, we report simple modifications of the small Pople-type Gaussian Type Orbital basis sets (3-21G, 3-21G*, 6-31G, 6-31G*), which correct their faulty behavior for the spin-state energies. We have investigated the basis sets for a set of thirteen first-row transition-metal complexes, for which reliable reference data have been obtained at the OPBE/TZ2P(STO) level. For several systems we have used single and double spin-contamination corrections to avoid ambiguity of the results due to spin-contamination, i.e. the energies and geometries were obtained for the pure spin states. The spin ground-states as predicted by the spin-state corrected GTO basis sets (s6-31G, s6-31G*) are in complete agreement with the reference STO data, while those of the original basis sets and a recent modification by Baker and Pulay (m6-31G*) are not for all cases. The spin-state corrected GTO basis sets also improve upon the original and modified basis sets for the accuracy of geometry optimization, while the accuracy of the vibrational frequencies is as good or better. At a limited additional cost, one therefore obtains very reliable results for these important spin-state energies |
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