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Newton, M.D.1
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15
-
-
85034501887
-
-
The numerical results in Ref. 4 also indicate that the proximity to resonance is a factor that determines the accuracy of the tight binding approximation
-
The numerical results in Ref. 4 also indicate that the proximity to resonance is a factor that determines the accuracy of the tight binding approximation.
-
-
-
-
18
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0003217338
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Scanning Tunneling Microscopy and Its Application
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Springer Verlag, Berlin
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Nitzan, A.7
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24
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0000031946
-
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and references therein
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See, e.g., C. Joachim, J. K. Gimzewski, R. R. Schlitter, and C. Chavy, Phys. Rev. Lett. 74, 2102 (1995), and references therein;
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33
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0000031946
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and references therein
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See C. Joachim, J. K. Gimzewski, R. R. Schlitter, and C. Chavy, Phys. Rev. Lett. 74, 2102 (1995), and references therein;
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Joachim, C.1
Gimzewski, J.K.2
Schlitter, R.R.3
Chavy, C.4
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34
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33645993207
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and references therein
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V. Mujica, M. Kemp, and M. A. Ratner, J. Chem. Phys. 101, 6849 (1994), and references therein;
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Mujica, V.1
Kemp, M.2
Ratner, M.A.3
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36
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2842602678
-
-
and references therein
-
M. P. Samanta, W. Tian, S. Datta, J. I. Henderson, and C. P. Kubiak, Phys. Rev. B 53, 7626 (1996), and references therein.
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Phys. Rev. B
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Samanta, M.P.1
Tian, W.2
Datta, S.3
Henderson, J.I.4
Kubiak, C.P.5
-
37
-
-
85034507937
-
-
A limiting case of this model was used before for analyzing bridge mediated electron transfer in Ref. 4
-
A limiting case of this model was used before for analyzing bridge mediated electron transfer in Ref. 4.
-
-
-
-
40
-
-
85034509809
-
-
note
-
rr′ between states of the same manifolds are nonzero but much smaller than those that mix states from the different manifolds, and are disregarded.
-
-
-
-
41
-
-
0031566913
-
-
2) see A. A. Stuchehrukhor, Chem. Phys. Lett. 265, 643 (1997). The correction to unity in the denominator can be disregarded under our model assumptions.
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(1997)
Chem. Phys. Lett.
, vol.265
, pp. 643
-
-
Stuchehrukhor, A.A.1
-
42
-
-
85034510896
-
-
note
-
-1 = L/2π is recognized as the density of momentum states in one dimension.
-
-
-
-
43
-
-
85034497448
-
-
l
-
l.
-
-
-
-
44
-
-
85034505063
-
-
note
-
The association of the Ṽ and ṼGṼ terms with "direct" and "indirect" contributions is to a large extent a matter of definition. In off-resonance situations, where the intermediate manifold {m} is not populated, also the second term could be viewed as direct.
-
-
-
-
47
-
-
0000850352
-
-
For applications to tunneling, see A. Mosyak, A. Nitzan, and R. Kosloff, J. Chem. Phys. 104, 1549 (1996);
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J. Chem. Phys.
, vol.104
, pp. 1549
-
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Mosyak, A.1
Nitzan, A.2
Kosloff, R.3
-
48
-
-
0030853033
-
-
A. Mosyak, P. Graf, I. Benjamin, and A. Nitzan, J. Phys. Chem. A 101, 429 (1997);
-
(1997)
J. Phys. Chem. A
, vol.101
, pp. 429
-
-
Mosyak, A.1
Graf, P.2
Benjamin, I.3
Nitzan, A.4
-
50
-
-
33645832116
-
-
J. Chem. Phys. 106, 1291 (1997);
-
(1997)
J. Chem. Phys.
, vol.106
, pp. 1291
-
-
-
51
-
-
85045535141
-
-
A. Haran, K. Kadyshevitch, H. Cohenn, R. Naaman, D. Evans, T. Seidman, and A. Nitzan, Chem. Phys. Lett. 268, 475 (1977).
-
(1977)
Chem. Phys. Lett.
, vol.268
, pp. 475
-
-
Haran, A.1
Kadyshevitch, K.2
Cohenn, H.3
Naaman, R.4
Evans, D.5
Seidman, T.6
Nitzan, A.7
-
52
-
-
85034519110
-
-
note
-
λ|.
-
-
-
-
53
-
-
85034512954
-
-
Note that we anticipate here that z is purely imaginary
-
Note that we anticipate here that z is purely imaginary.
-
-
-
|