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Semi-empirical quantum chemistry methods are based on the Hartree-Fock formalism, but make many approximations and obtain some parameters from empirical data. They are very important in computational chemistry for treating large molecules where the full Hartree-Fock method without the approximations is too expensive. The use of empirical parameters appears to allow some inclusion of electron correlation effects into the methods.
Within the framework of Hartree-Fock calculations, some pieces of information (such as two-elecron integrals) are sometimes approximated or completely omitted. In order to correct for this loss, semi-empirical methods are parametrized, that is their results are fitted by a set of parameters, normally in such a way as to produce results that best agree with experimental data, but sometimes to agree with ab initio results.
Semi-empirical methods follow what are often called empirical methods where the two-electron part of the Hamiltonian is not explicitly included. For π-electron systems, this was the Hückel method proposed by Erich Hückel [1] [2] [3] For all valence electron systems, the Extended Hückel method was proposed by Roald Hoffmann. [4]
Semi-empirical calculations are much faster than their ab initio counterparts. Their results, however, can be very wrong if the molecule being computed is not similar enough to the molecules in the database used to parametrize the method.
Semi-empirical calculations have been most successful in the description of organic chemistry, where only a few elements are used extensively and molecules are of moderate size.
As with empirical methods, we can distinguish methods that are:-
- restricted to pi-electrons. These method exist for the calculation of electronically excited states of polyenes, both cyclic and linear. These methods, such as the Pariser-Parr-Pople method (PPP), can provide good estimates of the pi-electronic excited states, when parameterized well. [5] [6] Indeed, for many years, the PPP method outperformed ab initio excited state calculations.
or those:-
- restricted to all valence electrons. These methods can be grouped into several groups:-
-
- Methods whose primary aim is to predict the geometries of coordination compounds, such as Sparkle/AM1, available for lanthanide complexes.
the latter being by far the largest group of methods.
The table below shows some software packages that carry out semi-empirical methods, indicating the other methods that they include where applicable.
| Package | Molecular Mechanics | Hartree-Fock | Post-Hartree-Fock methods | Density Functional Theory | |
| AMPAC | N | N | N | N | |
| GAMESS (UK) | N | Y | Y | Y | |
| GAMESS (US) | N | Y | Y | Y | |
| GAUSSIAN | Y | Y | Y | Y | |
| MOLCAS | Y | Y | Y | Y | |
| MOPAC | N | N | N | N | |
| PC GAMESS | Y | Y | Y | Y | |
| PQS | Y | Y | Y | Y | Y |
| VASP | N | Y | N | Y |
See also
References
- ^ E. Hückel, Zeitschrift für Physik, 70, 204, (1931); 72, 310, (1931); 76, 628 (1932); 83, 632, (1933)
- ^ Hückel Theory for Organic Chemists, C. A. Coulson, B. O'Leary and R. B. Mallion, Academic Press,1978.
- ^ Andrew Streitwieser, Molecular Orbital Theory for Organic Chemists, Wiley, New York, (1961)
- ^ R. Hoffmann, Journal of Chemical Physics, 39, 1397, (1963)
- ^ R. Pariser and R. Parr, Journal of Chemical Physics, 21, 466, 767, (1953)
- ^ J. A. Pople, Transactions of the Faraday Society, 49, 1375, (1953)
- ^ J. Pople and D. Beveridge, Approximate Molecular Orbital Theory, McGraw-Hill, 1970.
- ^ Ira Levine, Quantum Chemistry, Prentice Hall, 4th edition, (1991), pg 579 - 580
- ^ C. J. Cramer, Essentials of Computational Chemistry, Wiley, Chichester, (2002), pg 126 - 131
- ^ J. J. P. Stewart, Reviews in Computational Chemistry, Volume 1, Eds. K. B. Lipkowitz and D. B. Boyd, VCH, New York, 45, (1990)
- ^ M. Zerner, Reviews in Computational Chemistry, Volume 2, Eds. K. B. Lipkowitz and D. B. Boyd, VCH, New York, 313, (1991)
- ^ Nanda, D. N. and Jug, K., Theoretica Chimica Acta, 57, 95, (1980)
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