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7
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Chastanet, G.6
Marchivie, M.7
Goux-Capes, L.8
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15244351465
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Simaan, A.J.1
Boillot, M.-L.2
Carrasco, R.3
Cano, J.4
Girerd, J.-J.5
Mattioli, T.A.6
Ensling, J.7
Spiering, H.8
Gütlich, P.9
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44
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75749103563
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Note
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LS-IS)
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58
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75749124101
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Note
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The same idea as the B3LYP** functional was reported by Harvey and his collaborators. They proposed the idea to decrease the contribution of the HF exchange and reported that the B3PW91** functional reproduces well the energy difference between the singlet and the triplet state. 36c
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74
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75749103969
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The linear internal technique is believed to present the upper limit of potential energy barriers
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The linear internal technique is believed to present the upper limit of potential energy barriers
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77
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0141704726
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Gaussian, Inc., Wallingford, CT
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M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, J. A. Montgomery, Jr., T. Vreven, K. N. Kudin, J. C. Burant, J. M. Millam, S. S. Iyengar, J. Tomasi, V. Barone, B. Mennucci, M. Cossi, G. Scalmani, N. Rega, G. A. Petersson, H. Nakatsuji, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, M. Klene, X. Li, J. E. Knox, H. P. Hratchian, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. Ochterski, P. Y. Ayala, K. Morokuma, G. A. Voth, P. Salvador, J. J. Dannenberg, V. G. Zakrzewski, S. Dapprich, A. D. Daniels, M. C. Strain, O. Farkas, D. K. Malick, A. D. Rabuck, K. Raghavachari, J. B. Foresman, J. V. Ortiz, Q. Cui, A. G. Baboul, S. Clifford, J. Cioslowski, B. B. Stefanov, G. Liu, A. Liashenko, P. Piskorz, I. Komaromi, R. L. Martin, D. J. Fox, T. Keith, M. A. Al-Laham, C. Y. Peng, A. Nanayakkara, M. Challacombe, P. M. W. Gill, B. G. Johnson, W. Chen, M. W. Wong, C. Gonzalez and J. A. Pople, GAUSSIAN 03 (Revision D.2), Gaussian, Inc., Wallingford, CT, 2004
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(2004)
GAUSSIAN 03 (Revision D.2)
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Frisch, M.J.1
Trucks, G.W.2
Schlegel, H.B.3
Scuseria, G.E.4
Robb, M.A.5
Cheeseman, J.R.6
Montgomery Jr., J.A.7
Vreven, T.8
Kudin, K.N.9
Burant, J.C.10
Millam, J.M.11
Iyengar, S.S.12
Tomasi, J.13
Barone, V.14
Mennucci, B.15
Cossi, M.16
Scalmani, G.17
Rega, N.18
Petersson, G.A.19
Nakatsuji, H.20
Hada, M.21
Ehara, M.22
Toyota, K.23
Fukuda, R.24
Hasegawa, J.25
Ishida, M.26
Nakajima, T.27
Honda, Y.28
Kitao, O.29
Nakai, H.30
Klene, M.31
Li, X.32
Knox, J.E.33
Hratchian, H.P.34
Cross, J.B.35
Bakken, V.36
Adamo, C.37
Jaramillo, J.38
Gomperts, R.39
Stratmann, R.E.40
Yazyev, O.41
Austin, A.J.42
Cammi, R.43
Pomelli, C.44
Ochterski, J.45
Ayala, P.Y.46
Morokuma, K.47
Voth, G.A.48
Salvador, P.49
Dannenberg, J.J.50
Zakrzewski, V.G.51
Dapprich, S.52
Daniels, A.D.53
Strain, M.C.54
Farkas, O.55
Malick, D.K.56
Rabuck, A.D.57
Raghavachari, K.58
Foresman, J.B.59
Ortiz, J.V.60
Cui, Q.61
Baboul, A.G.62
Clifford, S.63
Cioslowski, J.64
Stefanov, B.B.65
Liu, G.66
Liashenko, A.67
Piskorz, P.68
Komaromi, I.69
Martin, R.L.70
Fox, D.J.71
Keith, T.72
Al-Laham, M.A.73
Peng, C.Y.74
Nanayakkara, A.75
Challacombe, M.76
Gill, P.M.W.77
Johnson, B.G.78
Chen, W.79
Wong, M.W.80
Gonzalez, C.81
Pople, J.A.82
more..
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80
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75749139541
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If the instability exists in the closed-shell singlet state, alternatively, we carried out the unrestricted calculations. At the singlet equilibrium geometry, there is no instability
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If the instability exists in the closed-shell singlet state, alternatively, we carried out the unrestricted calculations. At the singlet equilibrium geometry, there is no instability
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81
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0038435850
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Swiss Center for Scientific Computing, Manno, Switzerland
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P. Flükiger, H. P. Lüthi, S. Portmann and J. Weber, MOLEKEL 4.3, Swiss Center for Scientific Computing, Manno, Switzerland, 2000-2002
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(2000)
MOLEKEL 4.3
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Flükiger, P.1
Lüthi, H.P.2
Portmann, S.3
Weber, J.4
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83
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75749146860
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Note
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LS = 0.77-0.61 = 0.16 Å for Fe(ii) ion and 0.645-0.55 = 0.095 Å for Fe(iii) ion. 50b
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85
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75749153099
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Note
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-1 (0.04 eV))
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89
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75749154258
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Note
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2+, the spin contamination occurs to some extent in the singlet and the triplet states bearing the quintet equilibrium geometry (Fig. S12C). To avoid the spin contamination, we carried out restricted DFT calculations of the singlet state and restricted open-shell DFT calculations of the triplet state bearing the quintet geometry. However, the potential energy surfaces do not change very much (Fig. S13); thus, the discussion based on the PESs of Fig. 3 does not change at all. See Fig. S13 and its detailed discussion in the ESI, p. 29
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90
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75749118102
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3+ is much less than in its Fe(II) analogue; the difference between the S**2 expectation value and the ideal one is less than 0.12 for all spin states
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3+ is much less than in its Fe(II) analogue; the difference between the S**2 expectation value and the ideal one is less than 0.12 for all spin states
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