1996
DOI: 10.1103/physrevlett.76.2690
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Classical Chaos as an Environment for Dissipation

Abstract: We study an isolated three-dimensional system composed of a slow one-freedom system of interest interacting with a soft-chaotic environment. We present numerical evidence that the averaged motion of the slow system is dissipative, though not exactly governed by the Langevin equation. An analytical reasoning is proposed to explain the results, circumventing the unsufficiency of the adiabatic hypothesis.

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Cited by 12 publications
(25 citation statements)
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References 10 publications
(13 reference statements)
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“…Notice that the quantity E o (t) is very different from E o ( z , p z ), which is the energy of the average trajectory, considered in [3].…”
Section: Application To the Modelmentioning
confidence: 99%
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“…Notice that the quantity E o (t) is very different from E o ( z , p z ), which is the energy of the average trajectory, considered in [3].…”
Section: Application To the Modelmentioning
confidence: 99%
“…Low dimensional chaotic systems can, under appropriate circumstances, play the role of thermodynamical heat baths [1,2,3,4,5,6,7]. If a slow system with few degrees of freedom is weakly coupled to a fast chaotic system, the slow system's average trajectory can dissipate energy into the chaotic one at short times.…”
Section: Introductionmentioning
confidence: 99%
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“…The spectral function, which is related to the distribution of frequencies of the normal modes, can be chosen to model several types of thermal baths [3][4][5]. Other representations of the environment have also been explored, from spin systems [6] (or two-level atoms) to chaotic systems [7][8][9][10][11]. The latter is particularly important to model coupling to small external systems where the chaotic nature of the trajectories compensates for the small number of degrees of freedom in the decay of correlation functions.…”
Section: Introductionmentioning
confidence: 99%