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Search Results: 1 - 10 of 340477 matches for " H. R. Jauslin "
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Critical Attractor and Universality in a Renormalization Scheme for Three Frequency Hamiltonian Systems
C. Chandre,H. R. Jauslin
Physics , 1998, DOI: 10.1103/PhysRevLett.81.5125
Abstract: We study an approximate renormalization-group transformation to analyze the breakup of invariant tori for three degrees of freedom Hamiltonian systems. The scheme is implemented for the spiral mean torus. We find numerically that the critical surface is the stable manifold of a critical nonperiodic attractor. We compute scaling exponents associated with this fixed set, and find that they can be expected to be universal.
KAM--renormalization-group for Hamiltonian systems with two degrees of freedom
C. Chandre,H. R. Jauslin
Physics , 1998,
Abstract: We review a formulation of a renormalization-group scheme for Hamiltonian systems with two degrees of freedom. We discuss the renormalization flow on the basis of the continued fraction expansion of the frequency. The goal of this approach is to understand universal scaling behavior of critical invariant tori.
A Version of Thirring's Approach to the KAM Theorem for Quadratic Hamiltonians with Degenerate Twist
C. Chandre,H. R. Jauslin
Physics , 1998, DOI: 10.1063/1.532599
Abstract: We give a proof of the KAM theorem on the existence of invariant tori for weakly perturbed Hamiltonian systems, based on Thirring's approach for Hamiltonians that are quadratic in the action variables. The main point of this approach is that the iteration of canonical transformations on which the proof is based stays within the space of quadratic Hamiltonians. We show that Thirring's proof for nondegenerate Hamiltonians can be adapted to Hamiltonians with degenerate twist. This case, in fact, drastically simplifies Thirring's proof.
Strange attractor for the renormalization flow for invariant tori of Hamiltonian systems with two generic frequencies
C. Chandre,H. R. Jauslin
Physics , 1999, DOI: 10.1103/PhysRevE.61.1320
Abstract: We analyze the stability of invariant tori for Hamiltonian systems with two degrees of freedom by constructing a transformation that combines Kolmogorov-Arnold-Moser theory and renormalization-group techniques. This transformation is based on the continued fraction expansion of the frequency of the torus. We apply this transformation numerically for arbitrary frequencies that contain bounded entries in the continued fraction expansion. We give a global picture of renormalization flow for the stability of invariant tori, and we show that the properties of critical (and near critical) tori can be obtained by analyzing renormalization dynamics around a single hyperbolic strange attractor. We compute the fractal diagram, i.e., the critical coupling as a function of the frequencies, associated with a given one-parameter family.
Upper quantum Lyapunov Exponent and Anosov relations for quantum systems driven by a classical flow
O. Sapin,H. R. Jauslin,S. Weigert
Physics , 2005,
Abstract: We generalize the definition of quantum Anosov properties and the related Lyapunov exponents to the case of quantum systems driven by a classical flow, i.e. skew-product systems. We show that the skew Anosov properties can be interpreted as regular Anosov properties in an enlarged Hilbert space, in the framework of a generalized Floquet theory. This extension allows us to describe the hyperbolicity properties of almost-periodic quantum parametric oscillators and we show that their upper Lyapunov exponents are positive and equal to the Lyapunov exponent of the corresponding classical parametric oscillators. As second example, we show that the configurational quantum cat system satisfies quantum Anosov properties.
Time-optimal control of a two-level dissipative quantum system
D. Sugny,C. Kontz,H. R. Jauslin
Physics , 2007, DOI: 10.1103/PhysRevA.76.023419
Abstract: We propose an analysis of the time-optimal control of a dissipative two-level quantum system whose dynamics is governed by the Lindblad equation. This simple system allows one to use tools of geometric control theory and to construct its optimal synthesis, i.e. to determine the set of all the optimal trajectories starting from a given initial point. We study different processes such as conversion of a pure state into a mixed state and purification of a mixed state. In particular cases, we show that dissipation is not undesirable and can help accelerating the control.
Kolmogorov-Arnold-Moser Renormalization-Group Approach to the Breakup of Invariant Tori in Hamiltonian Systems
C. Chandre,M. Govin,H. R. Jauslin
Physics , 1998, DOI: 10.1103/PhysRevE.57.1536
Abstract: We analyze the breakup of invariant tori in Hamiltonian systems with two degrees of freedom using a combination of KAM theory and renormalization-group techniques. We consider a class of Hamiltonians quadratic in the action variables that is invariant under the chosen KAM transformations, following the approach of Thirring. The numerical implementation of the transformation shows that the KAM iteration converges up to the critical coupling at which the torus breaks up. By combining this iteration with a renormalization, consisting of a shift of resonances and rescalings of momentum and energy, we obtain a much more efficient method that allows to determine the critical coupling with high accuracy. This transformation is based on the physical mechanism of the breakup of invariant tori. We show that the critical surface of the transformation is the stable manifold of codimension one of a nontrivial fixed point, and we discuss its universality properties.
Kolmogorov-Arnold-Moser--Renormalization-Group Analysis of Stability in Hamiltonian Flows
M. Govin,C. Chandre,H. R. Jauslin
Physics , 1998, DOI: 10.1103/PhysRevLett.79.3881
Abstract: We study the stability and breakup of invariant tori in Hamiltonian flows using a combination of Kolmogorov-Arnold-Moser (KAM) theory and renormalization-group techniques. We implement the scheme numerically for a family of Hamiltonians quadratic in the actions to analyze the strong coupling regime. We show that the KAM iteration converges up to the critical coupling at which the torus breaks up. Adding a renormalization consisting of a rescaling of phase space and a shift of resonances allows us to determine the critical coupling with higher accuracy. We determine a nontrivial fixed point and its universality properties.
An Approximate KAM-Renormalization-Group Scheme for Hamiltonian Systems
C. Chandre,H. R. Jauslin,G. Benfatto
Physics , 1998, DOI: 10.1023/A:1004519514702
Abstract: We construct an approximate renormalization scheme for Hamiltonian systems with two degrees of freedom. This scheme is a combination of Kolmogorov-Arnold-Moser (KAM) theory and renormalization-group techniques. It makes the connection between the approximate renormalization procedure derived by Escande and Doveil, and a systematic expansion of the transformation. In particular, we show that the two main approximations, consisting in keeping only the quadratic terms in the actions and the two main resonances, keep the essential information on the threshold of the breakup of invariant tori.
Universality for the breakup of invariant tori in Hamiltonian flows
C. Chandre,M. Govin,H. R. Jauslin,H. Koch
Physics , 1998, DOI: 10.1103/PhysRevE.57.6612
Abstract: In this article, we describe a new renormalization-group scheme for analyzing the breakup of invariant tori for Hamiltonian systems with two degrees of freedom. The transformation, which acts on Hamiltonians that are quadratic in the action variables, combines a rescaling of phase space and a partial elimination of irrelevant (non-resonant) frequencies. It is implemented numerically for the case applying to golden invariant tori. We find a nontrivial fixed point and compute the corresponding scaling and critical indices. If one compares flows to maps in the canonical way, our results are consistent with existing data on the breakup of golden invariant circles for area-preserving maps.
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