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2
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0040307478
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J., and, Phys. Rep., 127 (1990)
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J.P. Bouchaud and A. Georges, Phys. Rep. 195, 127 (1990).A. Einstein, Ann. Phys. (Leipzig)17, 549 (1905).
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Ann. Phys. (Leipzig)
, vol.17
, pp. 549
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Bouchaud, P.1
Georges, A.2
Einstein, A.3
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14
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0000175360
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The general model, including an arbitrary initial distribution of both types of particles, can be studied in the context of interacting-particle systems, which have attracted considerable attention recently. Some of the models in this field are catalytic reactions mediated by a surface
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The general model, including an arbitrary initial distribution of both types of particles, can be studied in the context of interacting-particle systems, which have attracted considerable attention recently. Some of the models in this field are catalytic reactions mediated by a surface [R.M. Ziff, Phys. Rev. Lett.56, 2553 (1986);
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(1986)
Phys. Rev. Lett.
, vol.56
, pp. 2553
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Ziff, R.M.1
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15
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0010056851
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contact processes, and related models with absorbing states [see, e.g., edited by G. Deutsher, (Hiler, Bristol, 1980), 5
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P. Grassberger, Z. Phys. B47, 255 (1982)], contact processes, and related models with absorbing states [see, e.g., Percolation Structures and Processes, edited by G. Deutsher, Annals of the Israel Physical Society, (Hiler, Bristol, 1980), Vol. 5;
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(1982)
Z. Phys. B
, vol.47
, pp. 255
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Grassberger, P.1
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16
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0001387229
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J. Marro and R. Dickman, (Cambridge University Press, Cambridge, 1996)], branching annihilating random walks
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J. Marro and R. Dickman, Nonequilibrium Phase Transitions and Critical Phenomena (Cambridge University Press, Cambridge, 1996)], branching annihilating random walks [P. Grassberger, J. Phys. A17, L105 (1984);
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(1984)
J. Phys. A
, vol.17
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Grassberger, P.1
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18
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0001169936
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A+A→0 (diffusive annihilation of particles of one type)
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I. Jensen, J. Phys. A26, 3921 (1993)], A+A→0 (diffusive annihilation of particles of one type) [L. Peliti, J. Phys. A19, L365 (1986);
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(1986)
J. Phys. A
, vol.19
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Jensen, I.1
Peliti, L.2
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19
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85035226910
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A+B→0 (diffusive annihilation of particles of different species) and
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K. Kang and S. Redner, Phys. Rev. A30, 2833 (1984)], A+B→0 (diffusive annihilation of particles of different species) [D. Toussaint and F. Wilcsek, J. Chem. Phys.78, 2642 (1983);
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(1983)
J. Chem. Phys.
, vol.78
, pp. 2642
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Kang, K.1
Redner, S.2
Toussaint, D.3
Wilcsek, F.4
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26
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3843129853
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3592 (1993)], models of ballistic annihilation (i.e., the particles move with a given velocity distribution instead of randomly hopping at each time, and annihilating each other when they collide)
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71, 3592 (1993)], models of ballistic annihilation (i.e., the particles move with a given velocity distribution instead of randomly hopping at each time, and annihilating each other when they collide) [E. Ben-Naim, Phys. Rev. Lett.70, 1890 (1993);
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(1993)
Phys. Rev. Lett.
, vol.70
, pp. 1890
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Ben-Naim, E.1
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28
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0038642512
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and references therein], and models with traps [, and
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J. Piasecki, Phys. Rev. E51, 5535 (1995), and references therein], and models with traps [P. Grassberger and I. Procaccia, J. Chem. Phys.77, 6281 (1982);
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(1982)
J. Chem. Phys.
, vol.77
, pp. 6281
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Piasecki, J.1
Grassberger, P.2
Procaccia, I.3
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0000345559
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A study of our model in that framework will be addressed elsewhere [M.A. Muñoz, D.O. Martínez, P. Molinàs-Mata, and A.-L. Barabási (unpublished)
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A. Szabo, Phys. Rev. Lett.61, 2496 (1988)]. A study of our model in that framework will be addressed elsewhere [M.A. Muñoz, D.O. Martínez, P. Molinàs-Mata, and A.-L. Barabási (unpublished)].
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(1988)
Phys. Rev. Lett.
, vol.61
, pp. 2496
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Szabo, A.1
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85035230750
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We define time step as the time spent in reaching a nearest neighbor site at constant speed
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We define time step as the time spent in reaching a nearest neighbor site at constant speed.
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31
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85035236567
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Omitted end note
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Omitted end note.
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85035203126
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While the radius of the circle is not equal to the mean-square displacement, we expect that the two quantities scale with the same exponent, since the motion of the walker is bounded by the perimeter formed by the unvisited sites, which in the mean-field description corresponds to the circle
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While the radius of the circle is not equal to the mean-square displacement, we expect that the two quantities scale with the same exponent, since the motion of the walker is bounded by the perimeter formed by the unvisited sites, which in the mean-field description corresponds to the circle.
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33
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85035222189
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For a review, see A.-L. Barabási and H. E. Stanley, (Cambridge University Press, Cambridge, 1995);, edited by F. Family and T. Vicsek (World Scientific, Singapore, 1991)
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For a review, see A.-L. Barabási and H. E. Stanley, Fractal Concepts in Surface Growth (Cambridge University Press, Cambridge, 1995); Dynamics of Fractal Surfaces, edited by F. Family and T. Vicsek (World Scientific, Singapore, 1991).
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