-
1
-
-
0033548502
-
-
MEHTA A. D. et al., Science, 283 (1999) 1689.
-
(1999)
Science
, vol.283
, pp. 1689
-
-
Mehta, A.D.1
-
3
-
-
0034646568
-
-
MANDELKOW E. and HOENGER A., Curr. Opin. Cell Biol., 11 (1999) 34, for latest results see HOENGER A. et al., J. Mol. Biol., 297 (2000) 1087.
-
(2000)
J. Mol. Biol.
, vol.297
, pp. 1087
-
-
Hoenger, A.1
-
5
-
-
0007189090
-
-
note
-
-1) and K = 10 the relaxation time can be as short as 10s. Some care has to be taken as these results were obtained with kinesin attached to beads.
-
-
-
-
10
-
-
0007255679
-
-
For a Java applet of the simulation see http://www.ph.tum.de/~avilfan/relax.
-
-
-
-
12
-
-
0007258157
-
-
note
-
The case without explicit diffusion corresponds to the "standard" [10] dimer filling model and the diffusive case to the "head-on" dimer filling model [24, 25] with the final vacancy concentration 0.1233. The final configuration is independent of the asymmetry in the binding rates.
-
-
-
-
14
-
-
0000216110
-
-
BARES P.-A. and MOBILIA M., Phys. Rev. E, 59 (1999) 1996. Note that the described solution is derived for a parameter set which requires a fine tuning between diffusion, pair-creation and annihilation rate. In our model this relation is not fulfilled. But, this difference becomes irrelevant in the scaling limit, since their and our model can be mapped onto each other by introducing a short-ranged interaction between particles. See also PARK S.-C., PARK J.-M. and KIM D., Phys. Rev. E, 63 (2001) 057102 for a comment about the validity of the analytical approximation. The observed deviations, however, do not affect the scaling limit.
-
(1999)
Phys. Rev. E
, vol.59
, pp. 1996
-
-
Bares, P.-A.1
Mobilia, M.2
-
15
-
-
0035333240
-
-
BARES P.-A. and MOBILIA M., Phys. Rev. E, 59 (1999) 1996. Note that the described solution is derived for a parameter set which requires a fine tuning between diffusion, pair-creation and annihilation rate. In our model this relation is not fulfilled. But, this difference becomes irrelevant in the scaling limit, since their and our model can be mapped onto each other by introducing a short-ranged interaction between particles. See also PARK S.-C., PARK J.-M. and KIM D., Phys. Rev. E, 63 (2001) 057102 for a comment about the validity of the analytical approximation. The observed deviations, however, do not affect the scaling limit.
-
(2001)
Phys. Rev. E
, vol.63
, pp. 057102
-
-
Park, S.-C.1
Park, J.-M.2
Kim, D.3
-
18
-
-
0007189949
-
Reaction-diffusion mechanisms and quantum spin systems
-
Field Theoretical Tools for Polymer and Particle Physics, edited by MEYER-ORTMANNS H. and KLÜMPER A., Springer, Berlin
-
SCHÜTZ G., Reaction-diffusion mechanisms and quantum spin systems, in Field Theoretical Tools for Polymer and Particle Physics, edited by MEYER-ORTMANNS H. and KLÜMPER A., Lect. Not. Phys., Vol. 508 (Springer, Berlin) 1998.
-
(1998)
Lect. Not. Phys.
, vol.508
-
-
Schütz, G.1
-
21
-
-
0011773481
-
-
KREBS K., PFANMÜLLER M. P., WEHEFRITZ B. and HINRICHSEN H., J. Stat. Phys., 78 (1995) 1429.
-
(1995)
J. Stat. Phys.
, vol.78
, pp. 1429
-
-
Krebs, K.1
Pfanmüller, M.P.2
Wehefritz, B.3
Hinrichsen, H.4
|