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Chaotic Scattering

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Part of the book series: Applied Mathematical Sciences ((AMS,volume 173))

Abstract

Scattering is a fundamental tool for probing many physical and chemical processes. In a scattering experiment, particles are injected into the system and their characteristics after the scattering are recorded, from which many properties of the system can be revealed. In a general sense, scattering can be defined as a problem of obtaining various relations between some output variables characterizing the particles after the scattering versus some input variables characterizing the particles before the scattering. The relations are called scattering functions. In a regular scattering process, the functions are typically smooth, examples of which can be found in textbooks of classical mechanics. It has been realized, however, that there can be situations in which a scattering function may contain an uncountably infinite number of singularities. Near any of the singularities, an arbitrarily small change in the input variable can cause a large change in the output variable. This is a sensitive dependence on initial conditions that signifies the appearance of chaos. Scattering in this case is chaotic.

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Notes

  1. 1.

    In hyperbolic chaotic scattering, all periodic orbits are unstable, while in nonhyperbolic chaotic scattering, there are stable or neutrally stable periodic orbits and quasiperiodic orbits, which will be treated in Sects. 6.3 and 6.4.

  2. 2.

    A saddle-center bifurcation in a Hamiltonian system is equivalent to a saddle-node bifurcation in dissipative systems that is responsible, for instance, for the creation of periodic windows in a chaotic parameter regime.

  3. 3.

    See footnote 2.

  4. 4.

    The algebraic-decay law holds not only for two-degree-of-freedom Hamiltonian systems, but also for higher-dimensional systems [192, 381].

  5. 5.

    In higher-dimensional scattering systems, the energy surface is no longer isolated into regions enclosed by KAM surfaces. The chaotic set in this case forms a single integrated component on which a typical particle can execute Arnol’d diffusion. If the energy surface is unbounded, the particle decay still obeys the algebraic law [192]. The characteristic behavior of Arnol’d diffusion in which a particle hops from one well-defined region in the phase space to another closely resembles the penetration of Cantori in two-dimensional systems. This is expected to lead to multiple decay exponents measured over short intervals of time.

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Correspondence to Ying-Cheng Lai .

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© 2011 Springer Science+Business Media, LLC

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Lai, YC., Tél, T. (2011). Chaotic Scattering. In: Transient Chaos. Applied Mathematical Sciences, vol 173. Springer, New York, NY. https://doi.org/10.1007/978-1-4419-6987-3_6

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