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1
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85036206535
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E. Ott, Chaos in Dynamical Systems (Cambridge University, New York, 1993)
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E. Ott, Chaos in Dynamical Systems (Cambridge University, New York, 1993).
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2
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85036263863
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J.R. Dorfman, An Introduction to Chaos in Nonequilibrium Statistical Mechanics (Cambridge University, New York, 1999)
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J.R. Dorfman, An Introduction to Chaos in Nonequilibrium Statistical Mechanics (Cambridge University, New York, 1999).
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4
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85036141061
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M.C. Gutzwiller, Chaos in Classical and Quantum Physics (Springer-Verlag, New York, 1990)
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M.C. Gutzwiller, Chaos in Classical and Quantum Physics (Springer-Verlag, New York, 1990).
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13
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85036436582
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P. Deift, Orthogonal Polynomials and Random Matrices A Riemann-Hilbert Approach, Courant Lecture Notes in Mathematics, Vol. 3 (American Mathematical Society, Providence, Rhode Island, 2000)
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P. Deift, Orthogonal Polynomials and Random Matrices: A Riemann-Hilbert Approach, Courant Lecture Notes in Mathematics, Vol. 3 (American Mathematical Society, Providence, Rhode Island, 2000).
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14
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85036247041
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M.L. Mehta, Random Matrices, 2nd ed. (Academic, London, 1991)
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M.L. Mehta, Random Matrices, 2nd ed. (Academic, London, 1991).
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16
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0001664226
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B. Shklovskii, B. Shapiro, B.R. Sears, P. Lambradines, and H.B. Shore, Phys. Rev. B 47, 11 487 (1993).
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(1993)
Phys. Rev. B
, vol.47
, pp. 11 487
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Shklovskii, B.1
Shapiro, B.2
Sears, B.R.3
Lambradines, P.4
Shore, H.B.5
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25
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85036379716
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Occurrences of the latter case are systematically checked in our code and the corresponding trajectories are discarded
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Occurrences of the latter case are systematically checked in our code and the corresponding trajectories are discarded.
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26
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85036163679
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From a numerical point of view, one should mention that the present trajectory alone can be followed up to time (Formula presented) without trouble and also that at (Formula presented), the symplectic structure has been preserved better than (Formula presented) (relative). Of course, these behaviors are not qualitatively modified on changing either initial conditions or energy
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From a numerical point of view, one should mention that the present trajectory alone can be followed up to time (Formula presented) without trouble and also that at (Formula presented), the symplectic structure has been preserved better than (Formula presented) (relative). Of course, these behaviors are not qualitatively modified on changing either initial conditions or energy.
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27
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85036169863
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More precisely, trajectories having initial conditions in the two largest areas will perform the collision (backward in time) before returning to PSOS, whereas other areas are images of these largest areas by the Poincaré map (backward in time)
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More precisely, trajectories having initial conditions in the two largest areas will perform the collision (backward in time) before returning to PSOS, whereas other areas are images of these largest areas by the Poincaré map (backward in time).
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30
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85036367852
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(Formula presented)
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(Formula presented)
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