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The van der waals radii used in this study are taken from D. Freifelder, Physical Chemistry for Students of Biology and Chemistry (Science Books International, Boston, 1982), p. 60: H (1.2 Å), O (1.4 Å), and C (1.5 Å). The SiH (1.55 Å) and PO (1.84 Å) bond lengths are taken from D. F. Shriver, P. W. Atkins, and C. H. Langford, Inorganic Chemistry (Freeman and Company, New York, 1990), p. 68.
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Physical Chemistry for Students of Biology and Chemistry
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Freifelder, D.1
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38
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0004244010
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Freeman and Company, New York
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The van der waals radii used in this study are taken from D. Freifelder, Physical Chemistry for Students of Biology and Chemistry (Science Books International, Boston, 1982), p. 60: H (1.2 Å), O (1.4 Å), and C (1.5 Å). The SiH (1.55 Å) and PO (1.84 Å) bond lengths are taken from D. F. Shriver, P. W. Atkins, and C. H. Langford, Inorganic Chemistry (Freeman and Company, New York, 1990), p. 68.
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39.40 These surface states are energetically unfavorable in the electron transfer reactions considered in this study and are neglected in the calculations
-
39.40 These surface states are energetically unfavorable in the electron transfer reactions considered in this study and are neglected in the calculations.
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-
-
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49
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85037508356
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note
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app with a unit diode factor A, in Eq. (54).
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50
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85037513991
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Lewis group (private communication)
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Lewis group (private communication),
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51
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0022012846
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53
-
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0342663236
-
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The self-exchange electron transfer rate constant for the viologen system (S. Dai, thesis. University of Tennessee, 1990) is about one order higher than that of the Fc system [R. M. Neilson, G. E. MacManis, L. K. Safford, and M. J. Weaver, J. Chem. Phys. 93, 2152(1989)]. Since no temperature-dependence measurement was done for the viologen system, the reorganization energy is unknown and thus no conclusion can be drawn by comparing the self-exchange reactions.
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Neilson, R.M.1
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Weaver, M.J.4
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54
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0004227051
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Prentice-Hall, New Jersey
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G. L. Miessler and D. A. Tarr, Inorganic Chemistry (Prentice-Hall, New Jersey, 1999); A. Haaland, Acc. Chem. Res. 12, 415 (1979); J. Giordan, J. H. Moore, and J. A. Tossel, ibid. 19, 281 (1979); E. Rühl and A. P. Hitchcock, J. Am. Chem. Soc. 111, 5069 (1989).
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Miessler, G.L.1
Tarr, D.A.2
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33845561125
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G. L. Miessler and D. A. Tarr, Inorganic Chemistry (Prentice-Hall, New Jersey, 1999); A. Haaland, Acc. Chem. Res. 12, 415 (1979); J. Giordan, J. H. Moore, and J. A. Tossel, ibid. 19, 281 (1979); E. Rühl and A. P. Hitchcock, J. Am. Chem. Soc. 111, 5069 (1989).
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Haaland, A.1
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G. L. Miessler and D. A. Tarr, Inorganic Chemistry (Prentice-Hall, New Jersey, 1999); A. Haaland, Acc. Chem. Res. 12, 415 (1979); J. Giordan, J. H. Moore, and J. A. Tossel, ibid. 19, 281 (1979); E. Rühl and A. P. Hitchcock, J. Am. Chem. Soc. 111, 5069 (1989).
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0001743590
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G. L. Miessler and D. A. Tarr, Inorganic Chemistry (Prentice-Hall, New Jersey, 1999); A. Haaland, Acc. Chem. Res. 12, 415 (1979); J. Giordan, J. H. Moore, and J. A. Tossel, ibid. 19, 281 (1979); E. Rühl and A. P. Hitchcock, J. Am. Chem. Soc. 111, 5069 (1989).
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Rühl, E.1
Hitchcock, A.P.2
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85037501303
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note
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There is some arbitrariness of this definition of the surface density of electrons and the averaged coupling matrix element because the applied potential on different atom layers of the semiconductor are different. But because the coupling between the semiconductor atoms and the redox species decays fast with their distance (with a decay length in the order of 1 Å), and the applied potential varies slowly (with the band bending in the order of 100 nm), it is a good approximation to assume that the density of electrons is the same in the semiconductor surface region of present interest.
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