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0030873609
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34
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0001017874
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-
35
-
-
85034279122
-
-
The 3 and 4 bond analogues are structures 8-9 in ref 9b
-
The 3 and 4 bond analogues are structures 8-9 in ref 9b.
-
-
-
-
36
-
-
85034293136
-
-
note
-
v, ω) pairs have been found which generate excellent fits of the CT emission spectra.
-
-
-
-
38
-
-
85034305480
-
-
note
-
v and ω, a better choice for exploring the impact of individual parameters on |V| are S and ω. In this partitioning, the latter term only appears in the classical activation energy portion of eq 2, and the former appears in the nuclear tunneling factor.
-
-
-
-
39
-
-
85034300797
-
-
-1
-
-1.
-
-
-
-
43
-
-
84986492477
-
-
(a) Besler, B. H.; Merz, K. M., Jr.; Kollman, P. A. J. Comput. Phys. 1990, 11, 431.
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Besler, B.H.1
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-
45
-
-
85034275288
-
-
note
-
D = 3.2 Å for 1 and 2 in acetonitrile does not significantly alter the predicted temperature dependence or magnitude of ΔG.
-
-
-
-
46
-
-
85034296971
-
-
note
-
The calculated reorganization energies for a charged molecule are roughly inversely proportional to the solute atomic radii. The radius parameters used in the FDPB method were determined in the manner described for the computation of ΔG°.
-
-
-
-
47
-
-
85034306437
-
-
note
-
o was modeled.
-
-
-
-
51
-
-
85034304258
-
-
To be submitted for publication
-
Vath, P.; Zimmt, M. B. To be submitted for publication.
-
-
-
Vath, P.1
Zimmt, M.B.2
-
52
-
-
0000574687
-
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Gould, I. R.; Noukakis, D.; Gomez-Jahn, L.; Young, R. H.; Goodman, J. L.; Farid, S. Chem. Phys. 1993, 176, 439.
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Gould, I.R.1
Noukakis, D.2
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Young, R.H.4
Goodman, J.L.5
Farid, S.6
-
53
-
-
85034275402
-
-
o determine the slope
-
o determine the slope.
-
-
-
-
54
-
-
85034297341
-
-
The error bounds reported for the couplings were obtained by determining the range of |V| values in the boxed region of the contour plot
-
The error bounds reported for the couplings were obtained by determining the range of |V| values in the boxed region of the contour plot.
-
-
-
-
55
-
-
85034307927
-
-
o(295 K) obtained with method 1 for 1 and 2 in benzonitrile are almost identical
-
o(295 K) obtained with method 1 for 1 and 2 in benzonitrile are almost identical.
-
-
-
-
56
-
-
0001118846
-
-
(a) Oliver, A. M.; Craig, D. C.; Paddon-Row, M. N.; Verhoeven, J. W. Chem. Phys. Lett. 1988, 150, 366.
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Oliver, A.M.1
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Verhoeven, J.W.4
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60
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33845558202
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(e) Paddon-Row, M. N.; Patney, H. K.; Brown, R. S.; Houk, K. N. J. Am. Chem. Soc. 1981, 103, 3, 5575.
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Paddon-Row, M.N.1
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-
62
-
-
0001466425
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Gould, I. R.; Ege, D.; Moser, J. E.; Farid, S. J. Am. Chem. Soc. 1990, 112, 4290.
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-
63
-
-
85034275186
-
-
The electron-transfer reaction of 3 in THF is too close to thermoneutral to provide useful estimates of |V|. (See the discussion in section VII.)
-
The electron-transfer reaction of 3 in THF is too close to thermoneutral to provide useful estimates of |V|. (See the discussion in section VII.)
-
-
-
-
67
-
-
36549095460
-
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(d) Garg, A.; Onuchic, J. N.; Ambegaokar, V. J. Chem. Phys. 1985, 83, 4491.
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68
-
-
85034304483
-
-
Use of such rate constant models was explored, but the resulting |V| were only 20-30% smaller than those reported under method 1 in Table 3
-
(e) Use of such rate constant models was explored, but the resulting |V| were only 20-30% smaller than those reported under method 1 in Table 3.
-
-
-
-
69
-
-
0029638889
-
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Cave, R. J.; Newton. M. D.; Kumar, K.; Zimmt, M. B. J. Phys. Chem. 1995, 99, 17501.
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71
-
-
85034290273
-
-
See the Supporting Information for views of the DBA/solvent complexes studied with ab initio methods
-
See the Supporting Information for views of the DBA/solvent complexes studied with ab initio methods.
-
-
-
-
73
-
-
0030873609
-
-
(b) Kurnikov, I. V.; Zusman. L. D.; Kurnikova, M. G.; Farid, R. S.; Beratan, D. N. J. Am. Chem. Soc. 1997, 119, 5690.
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Kurnikov, I.V.1
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Farid, R.S.4
Beratan, D.N.5
-
74
-
-
85034280303
-
-
note
-
43b were introduced to improve the virtual orbital description of excited donor states. The 3-21G and 6-311G basis sets were used in the Hartree-Fock calculations. CIS (configuration interaction singles) on the molecules were also employed to obtain the electronic coupling data. In this case, the coupling was calculated from the energy splitting of the two lowest CIS eigenstates that corresponded to donor and acceptor states. The donor and acceptor energies were shifted into resonance by attaching point charges to the donor and acceptor groups. The 3-21G basis set was used for CIS calculations. The CIS results agreed to within 30% with those derived using the Hartree-Fock/effective Hamiltonian method.
-
-
-
-
76
-
-
3142560041
-
-
(b) Svaan, M.; Parker, V. D. Acta Chem. Scand., Ser. B 1984, 38, 751.
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(1984)
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Svaan, M.1
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78
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0001680417
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(a) Miller, J. R.; Paulson, B. P.; Bal, R.; Closs, G. L. J. Phys. Chem. 1995, 99, 6923.
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Miller, J.R.1
Paulson, B.P.2
Bal, R.3
Closs, G.L.4
|