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(h) Cramer, C. J.; Nash, J. J.; Squires, R. R. Chem. Phys. Lett 1997, 277, 311.
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(i) de Visser, S. P.; Filatov, M.; Shaik, S. Phys. Chem. Chem. Phys. 2000, 2, 5046.
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(l) Evangelista, F. A.; Allen, W. D.; Schaefer, H. F., III. J. Chem. Phys. 2007, 127, 24102.
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Evangelista, F.A.1
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(q) Karton, A.; Kaminker, I.; Martin, J. M. L. J. Phys. Chem. A 2009, 113, 7610.
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Karton, A.1
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Hoffmann, R.; Imamura, A.; Hehre, W. J. J. Am. Chem. Soc. 1968, 90, 1499.
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Wei, H.1
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Smart, B.E.4
Borden, W.T.5
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For recent reviews of VB theory, see: (a)
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For recent reviews of VB theory, see: (a) Shaik, S.; Shurki, A.; Danovich, D.; Hiberty, P. C. Chem. Rev. 2001, 107, 1501-1539.
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Chem. Rev.
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Shaik, S.1
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Song, L. C.; Mo, Y. R.; Zhang, Q.; Wu, W. J. Comput. Chem. 2005, 26, 514.
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Song, L.C.1
Mo, Y.R.2
Zhang, Q.3
Wu, W.4
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Review
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(a) Review: Goddard, W. A., III; Dunning, T. H.; Hunt, W. J.; Hay, P. J. Acc. Chem. Res. 1973, 6, 368.
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Acc. Chem. Res.
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Iii, G.W.A.1
Dunning, T.H.2
Hunt, W.J.3
Hay, P.J.4
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33846788241
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Gaussian, Inc., Wallingford CT, The full list of authors is given in the Supporting Information.
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Gaussian 03, Revision D.02, Frisch, M. J. et al., Gaussian, Inc., Wallingford CT, 2004. The full list of authors is given in the Supporting Information.
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(2004)
Gaussian 03, Revision D.02
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Frisch, M.J.1
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40
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70349236728
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Review: Diradicals; Borden, W. T., Ed.; Wiley-Interscience: New York
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Review: Borden, W. T. In Diradicals; Borden, W. T., Ed.; Wiley-Interscience: New York, 1982; pp. 1-72.
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(1982)
, pp. 1-72
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Borden, W.T.1
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This information is available free of charge via the Internet at See any current masthead page for ordering information and Web access instructions.
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This information is available free of charge via the Internet at http:// pubs.acs.org. See any current masthead page for ordering information and Web access instructions.
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We are indebted to Professor Wei Wu for providing us with his program.
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We are indebted to Professor Wei Wu for providing us with his program.
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(a) Anderson, K.; Malmqvist, P. A.; Roos, B. O. J. Chem. Phys. 1992, 96, 1218.
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Anderson, K.1
Malmqvist, P.A.2
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(b) Andersson, K.; Malmqvist, P. A.; Roos, B. O.; Sadlej, A. J.; Wolinski, K. J. Chem. Phys. 1990, 94, 5483.
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Andersson, K.1
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Sadlej, A.J.4
Wolinski, K.5
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0141991885
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Molcas Version 6.4
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Molcas Version 6.4 Karlstrøm, G.; Lindh, R.; Malmqvist, P.-Å Roos, B. O.; Ryde, U.; Veryazov, V.; Widmark, P.-O.; Cossi, M.; Schimmelpfennig, B.; Neogrady, P.; Scijo, L. Comput. Mater. Sci. 2003, 28, 222.
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Karlstrøm, G.1
Lindh, R.2
Malmqvist, P.-A.3
Roos, B.O.4
Ryde, U.5
Veryazov, V.6
Widmark, P.-O.7
Cossi, M.8
Schimmelpfennig, B.9
Neogrady, P.10
Scijo, L.11
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12b At the ROHF geometry of the triplet, the energy of this hypothetical diradical is 1.9 kcal/mol below the VB energy of the triplet and 8.5 kcal/mol above the VB energy of the singlet, when the latter is computed at the GVB optimized geometry.
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12b At the ROHF geometry of the triplet, the energy of this hypothetical diradical is 1.9 kcal/mol below the VB energy of the triplet and 8.5 kcal/mol above the VB energy of the singlet, when the latter is computed at the GVB optimized geometry.
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S-T. See footnote e of Table 1.
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S-T. See footnote e of Table 1.
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49
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0002201691
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Reviews: (a) Davidson, E. R., Ed.; World Scientific: River Edge, NJ.
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Reviews: (a) Hiberty, P. C In Modern Electronic Structure Theory and Applications in Organic Chemistry; Davidson, E. R., Ed.; World Scientific: River Edge, NJ., 1997; pp. 289-367.
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(1997)
Modern Electronic Structure Theory and Applications in Organic Chemistry
, pp. 289-367
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Hiberty, P.C.1
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See, for example, refs. 5a, b, e, h, i, l, n, p, q.
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See, for example, refs. 5a, b, e, h, i, l, n, p, q.
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2, in this MO, the AO on A is hybridized away from the hydrogens, but the smaller lobe of the hybridized AO on A interacts in a bonding fashion with the 1s AOs of H. For more pictures and detailed descriptions, see, for example, (a) Prentice-Hall: Englewood Cliffs, NJ
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2, in this MO, the AO on A is hybridized away from the hydrogens, but the smaller lobe of the hybridized AO on A interacts in a bonding fashion with the 1s AOs of H. For more pictures and detailed descriptions, see, for example, (a) Borden, W. T. Modern Molecular Orbital Theory for Organic Chemists; Prentice-Hall: Englewood Cliffs, NJ, 1975; pp. 34-38.
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(1975)
Modern Molecular Orbital Theory for Organic Chemists
, pp. 34-38
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(b) Cherry, W.; Epiotis, N.; Borden, W. T. Acc. Chem. Res. 1977, 10, 167.
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(1977)
Acc. Chem. Res.
, vol.10
, pp. 167
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Cherry, W.1
Epiotis, N.2
Borden, W.T.3
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55
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* orbitais of the π bond between C(2) and C(3) gives rise to the SOMO, which has a node at C(2) and opposite phases at C(1) and C(3).
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* orbitais of the π bond between C(2) and C(3) gives rise to the SOMO, which has a node at C(2) and opposite phases at C(1) and C(3).
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A.
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A.
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S-T(GVB/ROHF).
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S-T(GVB/ROHF).
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S-T(TS) and is, presumably, due to the small, but visible, spatial reorientation of the AOs at C(1) and C(3) upon substitution of the more electronegative fluorine for hydrogen at C(2).
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S-T(TS) and is, presumably, due to the small, but visible, spatial reorientation of the AOs at C(1) and C(3) upon substitution of the more electronegative fluorine for hydrogen at C(2).
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(1998)
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