- Pariser–Parr–Pople method
In
molecular physics , the Pariser–Parr–Pople method applies semi-empiricalquantum mechanical methods to the quantitative prediction ofelectronic structure s and spectra, inmolecule s of interest in the field oforganic chemistry . Previous methods existed, such as the Hückel method which lead to theHückel's rule , but were limited in their scope, application and complexity, as is theExtended Huckel method .This approach was developed in the 1950s by
Rudolph Pariser withRobert Parr and co-developed byJohn Pople . [ R. Pariser and R. Parr,Journal of Chemical Physics , 21, 466, 767, (1953) ] [ J. A. Pople,Transactions of the Faraday Society , 49, 1375, (1953) ] It is essentially a more efficient method of finding reasonable approximations ofmolecular orbital s, useful in predicting physical and chemical nature of the molecule under study since molecular orbital characteristics have implications with regards to both the basic structure andreactivity of a molecule. This method used thezero-differential overlap (ZDO) approximation to reduce the problem to reasonable size and complexity but still required modern solid statecomputer s (as opposed topunch card orvacuum tube systems) before becoming fully useful for molecules larger thanbenzene .Originally, Pariser's goal of using this method was to predict the characteristics of complex organic dyes, but this was never realized. The method has wide applicability in precise prediction of electronic transitions, particularly lower
singlet transitions, and found wide application in theoretical and appliedquantum chemistry . The two basic papers on this subject were among the top five chemistry and physics citations reported in ISI, Current Contents 1977 for the period of 1961–1977 with a total of 2450 references.In contrast to the
Hartree-Fock -based semiempirical method counterparts (i.e:MOPAC ), the pi-electron theories have a very strongab initio basis. The PPP formulation is actually an approximate pi-electron effective operator, and the empirical parameters, in fact, include effectiveelectron correlation effects. A rigorous, ab initio theory of the PPP method is provided by diagrammatic, multi-reference, high order perturbation theory (Freed, Brandow, Lindgren, etc). (The exact formulation is non-trivial, and requires some field theory) Large scale ab initio calculations (Martin and Birge, Martin and Freed, Sheppard and Freed, etc.) have confirmed many of the approximations of the PPP model and explain why the PPP-like models work so well with such a simple formulation.References
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