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GRULER H., DEWALD U. and EBERHARDT M., Eur. Phys. J. B, 11 (1999) 187; KEMKEMER R., KLING D., KAUFMANN D. and GRULER H., Eur. Phys. J. E, 1 (2000) 215.
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Eur. Phys. J. E
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Kemkemer, R.1
Kling, D.2
Kaufmann, D.3
Gruler, H.4
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4
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0000798431
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Directed transport may arise even in the absence of a macroscopic bias, provided that both parity and time reversal symmetry are broken. CURIE P., J. Phys. (Paris) 3° Série (théorique et appliqué), III (1894) 393.
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(1894)
J. Phys. (Paris) 3° Série (Théorique et Appliqué)
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Curie, P.1
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6
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0001730998
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See, for example, VICSEK T., Phys. Rev. Lett., 75 (1995) 1226; CZIROK A., STANLEY H. E. and VICSEK T., J. Phys. A, 30 (1997) 1375; SHIMOYAMA N., SUGAWARA K., MIZUGUCHI T., HAYAKAWA Y. and SANO M., Phys. Rev. Lett., 76 (1996) 3870; HELBING D. and VICSEK T., New J. Phys., 1 (1999) 13.1-13.17 (http://www.njp.org/).
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Phys. Rev. Lett.
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Vicsek, T.1
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7
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0031557295
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See, for example, VICSEK T., Phys. Rev. Lett., 75 (1995) 1226; CZIROK A., STANLEY H. E. and VICSEK T., J. Phys. A, 30 (1997) 1375; SHIMOYAMA N., SUGAWARA K., MIZUGUCHI T., HAYAKAWA Y. and SANO M., Phys. Rev. Lett., 76 (1996) 3870; HELBING D. and VICSEK T., New J. Phys., 1 (1999) 13.1-13.17 (http://www.njp.org/).
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J. Phys. A
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Czirok, A.1
Stanley, H.E.2
Vicsek, T.3
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8
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0000451920
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See, for example, VICSEK T., Phys. Rev. Lett., 75 (1995) 1226; CZIROK A., STANLEY H. E. and VICSEK T., J. Phys. A, 30 (1997) 1375; SHIMOYAMA N., SUGAWARA K., MIZUGUCHI T., HAYAKAWA Y. and SANO M., Phys. Rev. Lett., 76 (1996) 3870; HELBING D. and VICSEK T., New J. Phys., 1 (1999) 13.1-13.17 (http://www.njp.org/).
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Phys. Rev. Lett.
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Shimoyama, N.1
Sugawara, K.2
Mizuguchi, T.3
Hayakawa, Y.4
Sano, M.5
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9
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0037852770
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See, for example, VICSEK T., Phys. Rev. Lett., 75 (1995) 1226; CZIROK A., STANLEY H. E. and VICSEK T., J. Phys. A, 30 (1997) 1375; SHIMOYAMA N., SUGAWARA K., MIZUGUCHI T., HAYAKAWA Y. and SANO M., Phys. Rev. Lett., 76 (1996) 3870; HELBING D. and VICSEK T., New J. Phys., 1 (1999) 13.1-13.17 (http://www.njp.org/).
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New J. Phys.
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Helbing, D.1
Vicsek, T.2
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5544293263
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TONER J. and TU Y., Phys. Rev. Lett., 75 (1995) 4326; TU Y., ULM M. and TONER J., Phys. Rev. Lett., 80 (1998) 4819; TONER J. and TU Y., Phys. Rev. E, 58 (1998) 4828.
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Phys. Rev. Lett.
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Toner, J.1
Tu, Y.2
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4244091140
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TONER J. and TU Y., Phys. Rev. Lett., 75 (1995) 4326; TU Y., ULM M. and TONER J., Phys. Rev. Lett., 80 (1998) 4819; TONER J. and TU Y., Phys. Rev. E, 58 (1998) 4828.
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Phys. Rev. Lett.
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Tu, Y.1
Ulm, M.2
Toner, J.3
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TONER J. and TU Y., Phys. Rev. Lett., 75 (1995) 4326; TU Y., ULM M. and TONER J., Phys. Rev. Lett., 80 (1998) 4819; TONER J. and TU Y., Phys. Rev. E, 58 (1998) 4828.
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Phys. Rev. E
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Toner, J.1
Tu, Y.2
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RAMASWAMY S. and SIMHA R. A., Phys. Rev. Lett., 89 (2002) 058101; Physica A, 306 (2002) 262.
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Physica A
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15
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0013234806
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note
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The absence of momentum conservation can most easily be realized by considering two-dimensional systems (either powders or living organisms) on a substrate. Shaken three-dimensional powders or active cells in bulk fluid will not be described by our model. On the other hand, 3d systems of active particles in a random, frozen, space-filling network as a gel would be.
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18
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0001320144
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HAGEN M. H. J., PAGONABARRAGA I., LOWE C. P. and FRENKEL D., Phys. Rev. Lett., 78 (1997) 3785.
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Phys. Rev. Lett.
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Hagen, M.H.J.1
Pagonabarraga, I.2
Lowe, C.P.3
Frenkel, D.4
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20
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0013185420
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cond-mat/9909306
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An object with some of the properties of temperature can probably still be defined at least for some aspects of the behaviour of disordered, weakly driven systems. See KURCHAN J., cond-mat/9909306 and ONO I. K., O'HERN C. S., LANGER S. A., LIU A. J. and NAGEL S. R., cond-mat/0110276.
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Kurchan, J.1
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21
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0013187634
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cond-mat/0110276
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An object with some of the properties of temperature can probably still be defined at least for some aspects of the behaviour of disordered, weakly driven systems. See KURCHAN J., cond-mat/9909306 and ONO I. K., O'HERN C. S., LANGER S. A., LIU A. J. and NAGEL S. R., cond-mat/0110276.
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Ono, I.K.1
O'Hern, C.S.2
Langer, S.A.3
Liu, A.J.4
Nagel, S.R.5
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23
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33645076860
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KIRKPATRICK T. R., COHEN E. G. D. and DORFMAN J. R., Phys. Rev. A, 26 (1982) 995; LAW B. M., SEGRÈ P. N., GAMMON R. W. and SENGERS J. V., Phys. Rev. A, 41 (1990) 816.
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(1982)
Phys. Rev. A
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Kirkpatrick, T.R.1
Cohen, E.G.D.2
Dorfman, J.R.3
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24
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0000435789
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KIRKPATRICK T. R., COHEN E. G. D. and DORFMAN J. R., Phys. Rev. A, 26 (1982) 995; LAW B. M., SEGRÈ P. N., GAMMON R. W. and SENGERS J. V., Phys. Rev. A, 41 (1990) 816.
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Phys. Rev. A
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Law, B.M.1
Segrè, P.N.2
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0034248755
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DAS D. and BARMA M., Phys. Rev. Lett., 85 (2000) 1602; DAS D., BARMA M. and MAJUMDAR S. N., Phys. Rev. E, 64 (2001) 046126; DROSSEL B. and KARDAR M., cond-mat/0204464.
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Phys. Rev. Lett.
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Das, D.1
Barma, M.2
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26
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DAS D. and BARMA M., Phys. Rev. Lett., 85 (2000) 1602; DAS D., BARMA M. and MAJUMDAR S. N., Phys. Rev. E, 64 (2001) 046126; DROSSEL B. and KARDAR M., cond-mat/0204464.
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Phys. Rev. E
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Das, D.1
Barma, M.2
Majumdar, S.N.3
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27
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0034248755
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cond-mat/0204464
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DAS D. and BARMA M., Phys. Rev. Lett., 85 (2000) 1602; DAS D., BARMA M. and MAJUMDAR S. N., Phys. Rev. E, 64 (2001) 046126; DROSSEL B. and KARDAR M., cond-mat/0204464.
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Drossel, B.1
Kardar, M.2
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30
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0035419475
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for a similar treatment of active proteins
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See MANNEVTLLE J.-B., BASSEREAU P., RAMASWAMY S. and PROST J., Phys. Rev. E, 64 (2001) 021908 for a similar treatment of active proteins.
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(2001)
Phys. Rev. E
, vol.64
, pp. 021908
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Mannevtlle, J.-B.1
Bassereau, P.2
Ramaswamy, S.3
Prost, J.4
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31
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0013185008
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note
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One could, more generally, consider terms involving higher powers of Q; however, once fluctuations in the amplitude S are neglected, all position-dependent pieces of such terms are proportional to nn, as is already true of the term linear in Q. Hence, adding such higher powers of Q to σ has no effect on the final form of the equations of motion in the nematic state, but rather, only changes the values of some phenomenological parameters. Thus our model already describes all active nematics on a substrate.
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33
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0013247898
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note
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T here to generalize the model to systems in d > 2, such as those mentioned in [8].
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34
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0013287245
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note
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For any d > 2, the long-time tails are integrable so that the assumption of simple diffusive behavior for R(t) is self-consistent. In d = 2, the tails and the diffusivities will acquire logarithmic corrections.
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