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We use "dynamical asymmetry" to describe the property of any noise of which the asymmetric effect is not attributed to its asymmetric probability distribution but to its dynamics. The first usage of the word appeared in T. Hondou and Y. Sawada, Report. No. adap-org/9512002; Europhys. Lett. 35, 313 (1996).
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Conservation of a chaotic determinism in a dynamical system which shows extensive spatiotemporal chaos was investigated in H. Chaté, Ph. Marcq, and P. Manneville, in Dynamical Systems and Chaos, edited by Y. Aizawa, S. Saito, and K. Shiraiwa (World Scientific, Singapore, 1995), p. 583.
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For example, R.P. Feynman, R.B. Leighton, and M. Sands, The Feynman Lectures in Physics (Addison-Wesley, Reading, 1966).
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M.O. Magnasco, Phys. Rev. Lett. 71, 1477 (1993); C.R. Doering, W. Horsthemke, and J. Riordan, ibid. 72, 2984 (1994); R.D. Astumian and M. Bier, ibid. 72, 1776 (1994); J. Rousselet, L. Salomé, A. Ajdari, and J. Prost, Nature 370, 446 (1994); L. Faucheux, L. Bourdieu, P. Kaplan, and A. Libchaber, Phys. Rev. Lett. 74, 1504 (1995); K. Sugawara (private communication).
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M.O. Magnasco, Phys. Rev. Lett. 71, 1477 (1993); C.R. Doering, W. Horsthemke, and J. Riordan, ibid. 72, 2984 (1994); R.D. Astumian and M. Bier, ibid. 72, 1776 (1994); J. Rousselet, L. Salomé, A. Ajdari, and J. Prost, Nature 370, 446 (1994); L. Faucheux, L. Bourdieu, P. Kaplan, and A. Libchaber, Phys. Rev. Lett. 74, 1504 (1995); K. Sugawara (private communication).
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M.O. Magnasco, Phys. Rev. Lett. 71, 1477 (1993); C.R. Doering, W. Horsthemke, and J. Riordan, ibid. 72, 2984 (1994); R.D. Astumian and M. Bier, ibid. 72, 1776 (1994); J. Rousselet, L. Salomé, A. Ajdari, and J. Prost, Nature 370, 446 (1994); L. Faucheux, L. Bourdieu, P. Kaplan, and A. Libchaber, Phys. Rev. Lett. 74, 1504 (1995); K. Sugawara (private communication).
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Chialvo, D.R.1
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A different way to characterize chaos from the correlation function was reported by P.M. Gade and R.E. Amritkar, Phys. Rev. A 45, 725 (1992).
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The origin of the discovery of the asymmetric effect of chaotic noise can be found in Ref. [15]
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The first analytical derivation, limited for the tent map, for the barrier crossing probability appeared in T. Hondou, J. Phys. Soc. Jpn. 63, 2014 (1994). The origin of the discovery of the asymmetric effect of chaotic noise can be found in Ref. [15].
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Hondou, T.1
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85087249581
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note
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c/2,..., for one barrier crossing event gives an example.
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38
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5344247034
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note
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If A<1, η*becomes a stable fixed point, where the map cannot generate a noisy time series. Therefore, the state of the edge of chaos, A = 1 + ε (ε≪1 ), maximizes the barrier crossing probability induced by the chaotic noise.
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40
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5344274334
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unpublished
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S. Tasaki (unpublished).
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Tasaki, S.1
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