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Schlegel, H.B.3
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Robb, M.A.5
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Dapprich, S.11
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Daniels, A.D.13
Kudin, K.N.14
Strain, M.C.15
Farkas, O.16
Tomasi, J.17
Barone, V.18
Cossi, M.19
Cammi, R.20
Mennucci, B.21
Pomelli, C.22
Adamo, C.23
Clifford, S.24
Ochterski, J.25
Petersson, G.A.26
Ayala, P.Y.27
Cui, Q.28
Morokuma, K.29
Malick, D.K.30
Rabuck, A.D.31
Raghavachari, K.32
Foresman, J.B.33
Cioslowski, J.34
Ortiz, J.V.35
Stefanov, B.B.36
Liu, G.37
Liashenko, A.38
Piskorz, P.39
Komaromi, I.40
Gomberts, R.41
Martin, R.L.42
Fox, D.J.43
Keith, T.A.44
Al-Laham, M.A.45
Peng, C.Y.46
Nanayakkara, A.47
Gonzalez, C.48
Challacombe, M.49
Gill, P.M.W.50
Johnson, B.G.51
Chen, W.52
Wong, M.W.53
Andres, J.L.54
Head-Gordon, M.55
Replogle, E.S.56
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more..
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12
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0348112697
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note
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Local density approaches typically underestimate the degree of charge localization. Hartree-Fock may overestimate localization somewhat. A comparison of different methods would need to be benchmarked against experiments and is beyond the scope of this work.
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13
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0003770889
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Oxford University Press: Oxford
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We take the direction of the dipole moment to be from negative to positive charge. following: Stone, A. J. The Theory of Intermolecular Forces; Oxford University Press: Oxford, 1996.
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(1996)
The Theory of Intermolecular Forces
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Stone, A.J.1
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14
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0346852088
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note
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Recall that we are concerned here with the ground-state configuration, not with the temporal response and switching transient.
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15
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0347482613
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note
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Although the Hartree - Fock self-consistent iteration is not guaranteed to produce the right excited state, in this case, the energy difference is dominated by the electrostatic interaction with the driver (see below), so it provides a reasonable approximation to the excitation energy.
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16
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0035470233
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For a recent review of Robin and Day classes in mixed-valence chemistry see: Demadis, K. D.; Hartshom, C. M.; Meyer, T. J. Chem. Rev. 2001, 101, 2655.
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(2001)
Chem. Rev.
, vol.101
, pp. 2655
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Demadis, K.D.1
Hartshom, C.M.2
Meyer, T.J.3
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18
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0035848255
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(b) Orlov, A.O.; Kummamuru, R. K.; Ramasubramaniam, R.; Toth, G.; Lent, C. S.; Bernstein, G. H.; Snider, G. L. Appl. Phys. Lett. 2001, 78, 1625.
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(2001)
Appl. Phys. Lett.
, vol.78
, pp. 1625
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Orlov, A.O.1
Kummamuru, R.K.2
Ramasubramaniam, R.3
Toth, G.4
Lent, C.S.5
Bernstein, G.H.6
Snider, G.L.7
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20
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0346221497
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note
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We again ignore the complications of attachment to a surface or to neighboring molecules, which would be necessary to realize a full molecular QCA system.
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21
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0348112696
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note
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Note that the definition of cell polarization in ref 1 is precisely the normalized quadrupole moment.
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