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Volumn 56, Issue 3, 2001, Pages 420-426

Relaxation kinetics of biological dimer adsorption models

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[No Author keywords available]

Indexed keywords


EID: 0035498152     PISSN: 02955075     EISSN: None     Source Type: Journal    
DOI: 10.1209/epl/i2001-00535-4     Document Type: Article
Times cited : (10)

References (27)
  • 1
    • 0033548502 scopus 로고    scopus 로고
    • MEHTA A. D. et al., Science, 283 (1999) 1689.
    • (1999) Science , vol.283 , pp. 1689
    • Mehta, A.D.1
  • 3
    • 0034646568 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • For a Java applet of the simulation see http://www.ph.tum.de/~avilfan/relax.
  • 12
    • 0007258157 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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 scopus 로고    scopus 로고
    • 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


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.