1986
DOI: 10.1103/physreva.33.4055
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Coexistence of conservative and dissipative behavior in reversible dynamical systems

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Cited by 115 publications
(68 citation statements)
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“…The local velocity of a surface point of an extended particle need not coincide with the fluid velocity that one would observe at this point in the absence of the particle. As a consequence, the volume of the state space spanned by the particle's degrees of freedom is no longer conserved by the dynamics, which, as a result may display attractors for stationary flow fields, in spite of the fact that the dynamics is reversible [12]. In general, several attractors will coexist.…”
mentioning
confidence: 99%
“…The local velocity of a surface point of an extended particle need not coincide with the fluid velocity that one would observe at this point in the absence of the particle. As a consequence, the volume of the state space spanned by the particle's degrees of freedom is no longer conserved by the dynamics, which, as a result may display attractors for stationary flow fields, in spite of the fact that the dynamics is reversible [12]. In general, several attractors will coexist.…”
mentioning
confidence: 99%
“…The Rimmer bifurcations have been observed earlier in conservative systems, e.g. in the appearance of two period-6 orbits in the H6non map [11], and in period-2 orbits in a Poincar6 section associated with a set of reversible non-Hamiltonian differential equations arising from laser physics [4,5]. In the second case dissipative features including the appearance of an attractor and a repeller have been observed.…”
Section: G(x)mentioning
confidence: 81%
“…For x-independent solutions system (14) reduces to that explored in [18]. In general, in the basis of new functions u ± (x, t) = u(x, t) ± v(x, t) system (14) decouples into two nonlinear Schrödinger equations [21,22] …”
Section: On the Physical Modelmentioning
confidence: 99%