-
1
-
-
0031003997
-
-
R. D. Astumian, Science 276, 917 (1997); S. Leibler, Nature (London) 370, 412 (1994).
-
(1997)
Science
, vol.276
, pp. 917
-
-
Astumian, R.D.1
-
2
-
-
0027956106
-
-
London
-
R. D. Astumian, Science 276, 917 (1997); S. Leibler, Nature (London) 370, 412 (1994).
-
(1994)
Nature
, vol.370
, pp. 412
-
-
Leibler, S.1
-
3
-
-
0000230973
-
-
C. R. Doering, W. Horstemke, and J. Riordan, Phys. Rev. Lett. 72, 2984 (1994); R. Bartussek, P. Reimann, and P. Hänggi, ibid. 76, 1166 (1996); F. Marchesoni, Phys. Lett. A 237, 126 (1998).
-
(1994)
Phys. Rev. Lett.
, vol.72
, pp. 2984
-
-
Doering, C.R.1
Horstemke, W.2
Riordan, J.3
-
4
-
-
4243064040
-
-
C. R. Doering, W. Horstemke, and J. Riordan, Phys. Rev. Lett. 72, 2984 (1994); R. Bartussek, P. Reimann, and P. Hänggi, ibid. 76, 1166 (1996); F. Marchesoni, Phys. Lett. A 237, 126 (1998).
-
(1996)
Phys. Rev. Lett.
, vol.76
, pp. 1166
-
-
Bartussek, R.1
Reimann, P.2
Hänggi, P.3
-
5
-
-
0001212022
-
-
C. R. Doering, W. Horstemke, and J. Riordan, Phys. Rev. Lett. 72, 2984 (1994); R. Bartussek, P. Reimann, and P. Hänggi, ibid. 76, 1166 (1996); F. Marchesoni, Phys. Lett. A 237, 126 (1998).
-
(1998)
Phys. Lett. A
, vol.237
, pp. 126
-
-
Marchesoni, F.1
-
9
-
-
85034123923
-
-
note
-
The stepwise propagation of the AM pulses makes a quantitative interpretation of our simulation results easier. Anyway, we checked that thermal conveyers work effectively in the continuum limit m→t/Δt, as well.
-
-
-
-
13
-
-
0003577846
-
-
Dover, London
-
F. R. N. Nabarro, Theory of Crystal Dislocations (Dover, London, 1982); A. V. Granato and K. Lücke, in Physical Acoustics (Academic, New York, 1966), Vol. IVA, p. 225.
-
(1982)
Theory of Crystal Dislocations
-
-
Nabarro, F.R.N.1
-
14
-
-
85010527721
-
-
Academic, New York
-
F. R. N. Nabarro, Theory of Crystal Dislocations (Dover, London, 1982); A. V. Granato and K. Lücke, in Physical Acoustics (Academic, New York, 1966), Vol. IVA, p. 225.
-
(1966)
Physical Acoustics
, vol.4 A
, pp. 225
-
-
Granato, A.V.1
Lücke, K.2
-
16
-
-
0043283603
-
-
0/D) and k = 0,1. In the opposite limit, the perturbation caused by a traveling AM pulse spreads out over many substrate cells, thus forming an exponentially decaying trail. For Δt→0 a new adiabatic limit is recovered, where the effect of the time-dependent AM perturbation is equivalent to a static rescaling of the potential parameters - see, e.g., P. Jung, Phys. Rep. 65, 234 (1993).
-
(1993)
Phys. Rep.
, vol.65
, pp. 234
-
-
Jung, P.1
-
17
-
-
0039065101
-
-
L. Gammaitoni, P. Hänggi, P. Jung, and F. Marchesoni, Rev. Mod. Phys. 70, 223 (1998).
-
(1998)
Rev. Mod. Phys.
, vol.70
, pp. 223
-
-
Gammaitoni, L.1
Hänggi, P.2
Jung, P.3
Marchesoni, F.4
-
18
-
-
0038086544
-
-
M. Löcher, D. Cigna, E. R. Hunt, G. A. Johnson, F. Marchesoni, L. Gammaitoni, M. E. Inchiosa, and A. R. Bulsara, Chaos 8, 604 (1998).
-
(1998)
Chaos
, vol.8
, pp. 604
-
-
Löcher, M.1
Cigna, D.2
Hunt, E.R.3
Johnson, G.A.4
Marchesoni, F.5
Gammaitoni, L.6
Inchiosa, M.E.7
Bulsara, A.R.8
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