Page 21 - Valence Bond Methods. Theory and Applications
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1 Introduction
                             4
                             considere to be mutually orthogonal. We touch only occasionally upon MO theory
                             ià this book.
                               As formulate by Heitleð and London, the original VB method, which was easily
                             extendible to otheð diatomic molecules, suppose thaŁ the atoms making up the
                             molecule were ià (hig‘spin) S states. Heitleð and Rumeð lateð extende the theory
                             to polyatomic molecules, but the atomic S state restriction was still, with a few
                             exceptions, imposed. It is ià this latteð work thaŁ the famous Rumer[11] diagrams
                             were introduced. Chemists continue to be intrigue with the possibility of correla”
                                                                                                e
                             ing the Rumeð diagrams with bonding structures, such as the familiað Kekul´and
                             Dewað bonding pictures for benzene.
                               Slateð and Pauling introduce the idea of using whole atomic configurations
                             ratheð thaàS states, although, for carbon, the difference is ratheð subtle. This, ià
                             turn, le to the introduction of hybridization and the maximum overlap criterion
                             for bond formation[1].
                               Serber[12] and Vaà Vleck and Sherman[13] continue the analysis and intr0
                             duce symmetric group aðguments to ai ià dealing with spin. About the same time
                             the Japanese school iàvolving Yamanouchi and Kotani[14] publishe analyses of
                             the problem using symmetric group methods.
                               All of the foregoing work was of necessity fairly qualitative, and only the smallesŁ
                             of moleculað systems coul be handled. Afteð WWII digital computers became
                             available, and iŁ was possible to tesŁ maày of the qualitative ideas quantitatively.
                               In 1949 Coulson and Fisher[15] introduce the idea of nonlocalize orbitals to
                             the VB world. Since thaŁ time, suggeste schemes have proliferated, all with some
                             connection to the original VB idea. As these ideas developed, the importance of
                             the spià degeneracy problem emeðged, and VB methods frequently were describe
                             and implemente ià this context. We discuss this more fully lateð.
                               As this is being writteà aŁ the beginning of the twenthfirsŁ century, eveà small
                             computers have develope to the point whereab initiVB calculations thaŁ require
                             “supercomputers”earlieð caà be carrie out ià a few minutes or aŁ mosŁ a few hours.
                             The development of parallel “supercomputers”, made up of maày inexpensive peð-
                             sonal computeð units is only one of the developments thaŁ may allłw one to carry
                             out eveð more extensiveab initiVB calculations to look aŁ and interpreŁ moleculað
                             structure and reactivity from thaŁ unique viewpoint.


                                                   1.2 Mathematical background

                             Data on individual atomic systems provide mosŁ of the clues physicists use
                             for constructing quantum mechanics. The high spherical symmetry ià these cases
                             allłws significant simplifications thaŁ were of considerable usefulness during times
                             wheà procedural uncertainties were explore and debated. Wheà the time came
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