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7
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2942598393
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9
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F. W. Bobrowicz and W. A. Goddard, in Modern Theoretical Chemistry, ed. H. F. Schaefer III, Plenum Press, New York, 1977, ch. 4.
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Bobrowicz, F.W.1
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12
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33745044263
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MCQDPT2 (multi-configurational quasi-degenerate second-order perturbation theory) scheme by H. Nakano, J. Chem. Phys., 1993, 99, 7983, was used as implemented in GAMESS, ref. 12.
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13
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0347170005
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15
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84893169025
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M. W. Schmidt, K. K. Baldridge, J. A. Boatz, S. T. Elbert, M. S. Gordon, J. J. Jensen, S. Koseki, N. Matsungag, K. A. Nguyen, S. Su, T. L. Windus, M. Dupuis and J. A. Montgomery, J. Comput. Chem., 1993, 14, 1347.
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Schmidt, M.W.1
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Su, S.10
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Montgomery, J.A.13
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17
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2942568495
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note
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We note that, with counter-cations, spin symmetry broken density functional theory with B3LYP functional (UB3LYP) does not predict the dimer to be formed. The potential surface is purely repulsive. Use of UB3LYP (or another local density functional) is inappropriate to describe non-local dispersion phenomena, as discussed in ref. 15.
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19
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2942594682
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note
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We note that the existence of a stable dimer was predicted based on MP3 calculations in ref. 7, in which the authors used "1/R" correction to remove electrostatic repulsion for a dianion. There, over-binding was predicted.
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20
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2942568565
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note
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-1.
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21
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2942598394
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note
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In the MO picture, bond order = 1/2* (number of electrons in bonding orbitals - number of electrons in antibonding Orbitals).
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22
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2942534898
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note
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2- π-dimer.
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