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note
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The phase and amplitude envelope of an EXAFS single scattering (SS) contribution is nearly identical and indistinguishable by the fitting routines for scatterers with atomic number Z and Z ± 1 located at the same distance from the absorber. Fe-O/N refers to a SS contribution from either O or N; however, the theoretical phase and amplitude parameters were calculated for an Fe-O path.
-
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-
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63
-
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33645601345
-
-
note
-
The Cu⋯Fe SS and MS paths are strongly correlated. The disorder in the MS path in solution is larger than that in the solid. This, in addition to the higher noise level in the solution data, increases the error bar on the metal-metal distance determination.
-
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64
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0000614585
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-
65
-
-
33645599414
-
-
note
-
+ with the Fe⋯Cu constrained at different values between 3.6 and 4.15 Å was calculated using the Jaguar program at the BP86 level of theory, resulting in an energy difference between the fully optimized structure and that with an Fe⋯Cu distance constrained at 3.7 Å of 7.1 kcal/mol. Details of these calculations are given in Supporting Information.
-
-
-
-
66
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33645605236
-
-
note
-
Coupling constants calculated with pure DFT methods are normally 2-3 times larger than the experimental values.
-
-
-
-
67
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-
33645587371
-
-
note
-
2-Cu plane.
-
-
-
-
68
-
-
33645583950
-
-
note
-
For this bonding description, the porphyrin is defined as the xy plane, with the z axis perpendicular to this plane and the z axis along the O-O vector.
-
-
-
-
69
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33645586302
-
-
note
-
+ to provide a better basis for comparison. Details are given in Supporting Information.
-
-
-
-
70
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33645608167
-
-
note
-
In the broken symmetry description (S = 0), each spin-up orbital is energetically degenerate with a spin-down electron on the opposite site of the molecule. Such spin-up and spin-down electrons are images of one another under inversion.
-
-
-
-
71
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0000160591
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Burstyn, J. N.; Roe, S. A.; Miksztal, A. R.; Shaevitz, B. A.; Lang, G.; Valentine, S. S. J. Am. Chem. Soc. 1988, 110, 1382-1388.
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Burstyn, J.N.1
Roe, S.A.2
Miksztal, A.R.3
Shaevitz, B.A.4
Lang, G.5
Valentine, S.S.6
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Selke, M.; Sisemore, M. F.; Valentine, S. S. J. Am. Chem. Soc. 1996, 118, 2008-2012.
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Selke, M.1
Sisemore, M.F.2
Valentine, S.S.3
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73
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33645586171
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note
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- model complex was also optimized using a larger basis set containing diffuse functions. In particular, the basis set 6-311+G* was used for Fe and O, and the basis set 6-31+G* was used for N, C, and H. The results are very similar to those presented here.
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74
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33845281785
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Vanatta, R. B.; Strouse, C. E.; Hanson, L. K.; Valentine, J. S. J. Am. Chem. Soc. 1987, 109, 1425-1434.
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(1987)
J. Am. Chem. Soc.
, vol.109
, pp. 1425-1434
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Vanatta, R.B.1
Strouse, C.E.2
Hanson, L.K.3
Valentine, J.S.4
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75
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0037388015
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Cramer, C. J.; Tolman, W. B.; Theopold, K. H.; Rheingold, A. L. Proc. Natl. Acad. Sci. U.S.A. 2003, 100, 3635-3640.
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(2003)
Proc. Natl. Acad. Sci. U.S.A.
, vol.100
, pp. 3635-3640
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Cramer, C.J.1
Tolman, W.B.2
Theopold, K.H.3
Rheingold, A.L.4
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77
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33645592656
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note
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36 The reported Fe⋯Cu of 3.4 Å has been reevaluated in this study, and the EXAFS data are fit with an Fe⋯Cu and Cu⋯Fe component of ∼3.97 Å. This difference is likely due to differences in sample preparation, as the EXAFS data in L6 are clearly different from those reported herein.
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78
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33645592396
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note
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Some contribution to the σ superexchange pathway is also present in β-193.
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