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Physical review. B, Condensed matter

Variational localized-site cluster expansions. IX. Many-body valence-bond theory

Douglas J. Klein

Published Jan 15, 1979• 17 citations
Publisher

Abstract

A cluster-expansion approach to constructing valence-bond wave functions is described, such that calculations even on many-body systems are possible. In addition, the valence-bond idea of electron pairing is extended to site pairing, or site coupling, even though the sites may involve many electrons and be of a higher spin multiplicity.
DOI
10.1103/physrevb.19.870

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The classical theory of chemical valence, first, is naturally formalized in mathematics in the area of graph theory and, second, finds an extension in quantum mechanics in terms of the Heitler–London–Pauling “valence-bond” (VB) theory. Thus, VB theory stands in a fairly unique position, although in quantum chemistry, there often has been a preference for the alternative (perhaps even “complementary”) molecular orbital (MO) theory, presumably in large part because of computational efficacy for general molecular structures. Indeed, as formulated by Pauling and others, VB theory was described as a configuration interaction (CI) problem when there were multiple relevant classical valence structures for the same molecular structure. Also, as now recognized, a direct assault on CI is computationally intensive, prone to size-inconsistency problems, and effectively limited to smaller systems—whereas indirect approaches, e.g., via wave-function cluster expansions or renormalization-group theory, often neatly avoid these problems. Thus, what is (and perhaps always has been) needed is “many-body” schemes for VB computations (as well as for higher-order MO-based approaches, too). Here, then, certain such many-body VB-amenable computational schemes are to be discussed, in the context of semiempirical (explicitly correlated) graphical models. The collection of models are described and interrelated in a fairly comprehensive systematic manner. A selection of many-body cluster expansion methods are then discussed with special reference to resonating VB wave functions and the fundamental graph-theoretic nature of the consequent problems (such as also are noted to arise in lattice-discretized statistical-mechanical problems, too). Some examples are described incorporating resonance among exponentially great numbers of VB structures as applied: for large icosahedral-symmetry fullerenic structures, for the (polyacetylenic) linear chain, and for ladderlike conjugated polymers. It is contended that practicable many-body VB-theoretic methods are now available, retaining clear links to classical chemical valence theory. Hopefully, too, these methods may soon find use beyond the semi-empirical framework. © 1997 John Wiley & Sons, Inc. Int J Quant Chem 65: 421–438, 1997
Abstract A general and systematic localized‐site cluster expansion is described. It provides simple physically appealing and computationally feasible wave function ansätze, as well as, via extension of the cluster expansion, a unique expression for general, possibly exact, wave functions. We show that a variety of matrix element evaluation techniques are available and that they are sometimes exact though relatively simple. These techniques often proceed in terms of computational time proportional to the number of different types of sites, rather than their total number. Thus it seems we have a new and viable many‐body theory, which is expected to be most accurate and most readily implementable when a physical picture with slightly perturbed localized sites is relevant.
The resonating-valence-bond (RVB) State with one localized state per site is a state in which correlations are important and therefore for its determination it is necessary to go beyond the one-determinant approximation. Although the number of one-electron space orbitals is equal to the number of electrons, N, the number of necessary determinants increases factorially with N, thus making a rigorous treatment of the correlation effects impracticable even for systems containing relatively small number of electrons. On the other hand, by introducing a many-electron spin function a coupled system of equations for one-electron localized non-orthogonal space orbitals and N-electron spin function can be obtained which can be solved in practice. In this procedure the main difficulty resides in the equation for the N-electron spin function. In this paper it is shown that a perturbation theory based on the decomposition of the spin system into clusters, when taken beyond the first order can, in general, offer a suitable method of mapping the results of numerical calculations of spin clusters onto the total system.