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Volumn 19, Issue 6, 1998, Pages 610-627

Natural resonance theory: II. Natural bond order and valency

Author keywords

Bond order; Natural resonance theory; Resonance theory; Valency

Indexed keywords


EID: 0742313022     PISSN: 01928651     EISSN: None     Source Type: Journal    
DOI: 10.1002/(SICI)1096-987X(19980430)19:6<610::AID-JCC4>3.0.CO;2-U     Document Type: Article
Times cited : (511)

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    • Reference 1(b), p. 255
    • (a) Bond length: L. Pauling, J. Am. Chem. Soc., 69, 542 (1947); Reference 1(b), p. 255; C. A. Coulson, Proc. R. Soc. London, A207, 91 (1951); C. A. Coulson and A. Golebiewski, Proc. Phys. Soc., 78, 1310 (1961); G. Grampp, M. Cebe, and E. Cebe, Z. Phys. Chem., 166, 93 (1990).
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    • Oxford University Press, Longon, particularly Chapter VI
    • Useful discussion of the nature of valency, electrovalency, and covalency from a historical perspective are given by N. V. Sidgwick, The Electronic Theory of Valency, Oxford University Press, Longon, 1929, particularly Chapter VI; C. A. Russell, History of Valency, University Press, Leicester, 1971.
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    • Useful discussion of the nature of valency, electrovalency, and covalency from a historical perspective are given by N. V. Sidgwick, The Electronic Theory of Valency, Oxford University Press, Longon, 1929, particularly Chapter VI; C. A. Russell, History of Valency, University Press, Leicester, 1971.
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    • note
    • In principle, one might have (e.g., for an excited state) higher occupancy of an antibond than of the corresponding bond, which would lead to a net negative contribution to formal bond order. However, this situation is not provided for in the present version of the NRT program.
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    • For a comprehensive description of computational methods and basis set designations used herein, see W. J. Hehre, L. Radom, P. v. R. Schleyer, and J. A Pople, Ab Initio Molecular Orbital Theory, John Wiley, New York, 1986. All wave function calculations were performed with the Gaussian 92 program system: M. J. Frisch, G. W. Trucks, M. Head-Gordon, P. M. W. Gill, M. W. Wong, J. B. Foresman, B. G. Johnson, H. B. Schlegel, M. A. Robb, E. S. Repogle, R. Gomperts, J. L. Andres, K. Raghavachari, J. S. Binkley, C. Gonzalez, R. L. Martin, D. J. Fox, D. J. Defrees, J. Baker, J. J. P. Stewart, and J. A. Pople, Gaussian 92, Revision A, Gaussian, Inc., Pittsburgh, 1992.
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    • max) ensures that only the most strongly delocalized systems will have more than a single reference structure.
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    • note
    • The default NRT expansions for these wave functions include about 20 additional structures (not shown) with smaller weightings ≥ 0.01%.
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    • The superficially high weight of "long bond" structures in earlier RT treatments can be attributed to the "overcorrelation" artifact of Heitler-London valence-bond wave functions; see R. McWeeny, Proc. R. Soc. London, A223, 63, 306 (1954).
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    • note
    • CF reported in references 20 (0.572, RHF/6-31+ + G** level) and 22 (0.616 RHF/6-311 + + G** level) is therefore puzzling.
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    • C is rather close to the NRT covalency (2.427) in this case, but the corresponding valencies for fluorine differ by almost a factor of two.


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