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18844386816
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edited by B.-L. HAO (World Scientific)
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JANOWSKY S. A. and LEBOWITZ J. L., Phys. Rev. A, 45 (1992) 618; SCHÜTZ G., J. Stat. Phys., 71 (1993) 471; MALLICK K., J. Phys. A, 29 (1996) 5375; DERRIDA B., in Statphys19, edited by B.-L. HAO (World Scientific) 1996; EVANS M. R., Europhys. Lett., 36 (1996) 13; KRUG J. and FERRARI P. A., J. Phys. A, 29 (1996) L213: BEN-NAIM E., KRAPIVKSY P. L. and REDNER S., Phys. Rev. E, 50 (1994) 822.
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JANOWSKY S. A. and LEBOWITZ J. L., Phys. Rev. A, 45 (1992) 618; SCHÜTZ G., J. Stat. Phys., 71 (1993) 471; MALLICK K., J. Phys. A, 29 (1996) 5375; DERRIDA B., in Statphys19, edited by B.-L. HAO (World Scientific) 1996; EVANS M. R., Europhys. Lett., 36 (1996) 13; KRUG J. and FERRARI P. A., J. Phys. A, 29 (1996) L213: BEN-NAIM E., KRAPIVKSY P. L. and REDNER S., Phys. Rev. E, 50 (1994) 822.
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JANOWSKY S. A. and LEBOWITZ J. L., Phys. Rev. A, 45 (1992) 618; SCHÜTZ G., J. Stat. Phys., 71 (1993) 471; MALLICK K., J. Phys. A, 29 (1996) 5375; DERRIDA B., in Statphys19, edited by B.-L. HAO (World Scientific) 1996; EVANS M. R., Europhys. Lett., 36 (1996) 13; KRUG J. and FERRARI P. A., J. Phys. A, 29 (1996) L213: BEN-NAIM E., KRAPIVKSY P. L. and REDNER S., Phys. Rev. E, 50 (1994) 822.
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JANOWSKY S. A. and LEBOWITZ J. L., Phys. Rev. A, 45 (1992) 618; SCHÜTZ G., J. Stat. Phys., 71 (1993) 471; MALLICK K., J. Phys. A, 29 (1996) 5375; DERRIDA B., in Statphys19, edited by B.-L. HAO (World Scientific) 1996; EVANS M. R., Europhys. Lett., 36 (1996) 13; KRUG J. and FERRARI P. A., J. Phys. A, 29 (1996) L213: BEN-NAIM E., KRAPIVKSY P. L. and REDNER S., Phys. Rev. E, 50 (1994) 822.
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0040851785
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note
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i to be binary, this does not to forbid the presence of more than one passenger at a site; we merely require that the extra passengers have no further effect on the dynamics.
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14
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0040257328
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note
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This is because the interchange of a fast-moving bus with a slower-moving bus in front also interchanges their velocities. This contrasts sharply with Id models where jamming is induced by quenched disorder [5].
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15
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0039665562
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note
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The relevance of the BRM to real buses is discussed further in [11].
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16
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0040257329
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note
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In an exact mapping from the dual model to the BRM, a particle attempts to hop to the left when the site to its left is updated. However, a more natural dynamics with no significant difference in behaviour is to update only particles [11].
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17
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0039665563
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note
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Note that this violates Galilean invariance, requiring a pipe or some other fixed reference frame to be present.
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19
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0040257245
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note
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The variance of the noise should strictly depend on β but since we are primarily interested in the effect of λ on the dynamics of the gap, we ignore this dependence.
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21
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0039665560
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note
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The MFM is an example of a zero-range process for which the steady state is given by a product measure.
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0000527995
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BENJAMIN S. C., JOHNSON N. F. and HUI P. M., J. Phys. A, 29 (1996) 3119; SCHAD-SCHNEIDER A. and SCHRECKENBERG M., Ann. Phys. (Leipzig), 6 (1997); 541 cond-mat/9709131 preprint, 1997.
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0031341817
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cond-mat/9709131 preprint, 1997
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BENJAMIN S. C., JOHNSON N. F. and HUI P. M., J. Phys. A, 29 (1996) 3119; SCHAD-SCHNEIDER A. and SCHRECKENBERG M., Ann. Phys. (Leipzig), 6 (1997); 541 cond-mat/9709131 preprint, 1997.
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Ann. Phys. (Leipzig)
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0000074440
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SASVÁRI M. and KERTÉSZ J., Phys. Rev. E, 56 (1997) 4104: EISENBLÄTTER B., SANTEN L., SCHADSCHNEIDER A. and SCHRECKENBERG M., Phys. Rev. E, 57 (1998) 1309; cond-mat/9706041 preprint, 1997.
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cond-mat/9706041 preprint
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SASVÁRI M. and KERTÉSZ J., Phys. Rev. E, 56 (1997) 4104: EISENBLÄTTER B., SANTEN L., SCHADSCHNEIDER A. and SCHRECKENBERG M., Phys. Rev. E, 57 (1998) 1309; cond-mat/9706041 preprint, 1997.
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