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North-Holland, Amsterdam, M.-J. Giannoni, A. Voros, J. Zinn-Justin, Proceedings of the LII Session of the Les Houches Summer School of Theoretical Physics
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Chaos and Quantum Physics, edited by M.-J. Giannoni, A. Voros, and J. Zinn-Justin, Proceedings of the LII Session of the Les Houches Summer School of Theoretical Physics (North-Holland, Amsterdam, 1991).
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Chaos and Quantum Physics
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2
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0003886232
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Cambridge University Press, Cambridge, G. Casati, B. V. Chirikov
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Quantum Chaos: Between Order and Disorder, edited by G. Casati and B. V. Chirikov (Cambridge University Press, Cambridge, 1995).
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Quantum Chaos: Between Order and Disorder
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3
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85037178575
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O. Bohigas, in Ref. c1
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O. Bohigas, in Ref. 1.
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5
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85037200317
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M. V. Berry, in Ref. c1
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M. V. Berry, in Ref. 1.
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10
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4043147183
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F. Cooper, J. Dawson, D. Meredith, and H. Shepard, Phys. Rev. Lett. 72, 1337 (1994);
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Phys. Rev. Lett.
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Cooper, F.1
Dawson, J.2
Meredith, D.3
Shepard, H.4
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F. Cooper, J. Dawson, S. Habib, Y. Kluger, D. Meredith, and H. Shepard, Physica D 83, 74 (1995).
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Physica D
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Cooper, F.1
Dawson, J.2
Habib, S.3
Kluger, Y.4
Meredith, D.5
Shepard, H.6
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13
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85037225120
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e-print chao-dyn/9511007
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T. C. Blum and H. T. Elze, e-print chao-dyn/9511007;
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Blum, T.C.1
Elze, H.T.2
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16
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33744518241
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The “closed time path” formalism, initially proposed by Schwinger in 1961, is appropriate to the study of the causal evolution of observables from given initial conditions. For such an initial value problem the boundary conditions are different from those of standard scattering theory. See, e.g
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The “closed time path” formalism, initially proposed by Schwinger in 1961, is appropriate to the study of the causal evolution of observables from given initial conditions. For such an initial value problem the boundary conditions are different from those of standard scattering theory. See, e.g., J. Schwinger, J. Math. Phys. 2, 407 (1961);
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(1961)
J. Math. Phys.
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Schwinger, J.1
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17
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4243563667
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references therein
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F. Cooper, S. Habib, Y. Kluger, E. Mottola, J. P. Paz, and P. R. Anderson, Phys. Rev. D 50, 2848 (1994) and references therein.
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Phys. Rev. D
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Cooper, F.1
Habib, S.2
Kluger, Y.3
Mottola, E.4
Paz, J.P.5
Anderson, P.R.6
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18
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0001322458
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F. Cooper, S. Habib, Y. Kluger, and E. Mottola, Phys. Rev. D 55, 6471 (1997).
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Phys. Rev. D
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, pp. 6471
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Cooper, F.1
Habib, S.2
Kluger, Y.3
Mottola, E.4
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21
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0000254113
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Due to the Hamiltonian character of the systems only two Lyapunov exponents are nonzero, and they are equal in modulus, λ and [Formula Presented] For a thorough discussion on Lyapunov exponents and the ergodic theory of chaos see
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Due to the Hamiltonian character of the systems only two Lyapunov exponents are nonzero, and they are equal in modulus, λ and -λ. For a thorough discussion on Lyapunov exponents and the ergodic theory of chaos see J.-P. Eckmann and D. Ruelle, Rev. Mod. Phys. 57, 617 (1987).
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Rev. Mod. Phys.
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Eckmann, J.-P.1
Ruelle, D.2
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22
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85037193458
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The minimum of the classical potential energy has been fixed to zero for each value of [Formula Presented]
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The minimum of the classical potential energy has been fixed to zero for each value of B.
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23
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85037199582
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Such intersections are referred to as homoclinic intersections. This mechanism that originates chaos near a perturbed separatrix was discovered by Poincaré: see, e.g., H. Poincaré, Les Méthodes Nouvelles de la Mécanique Celeste (Gauthier-Villars, Paris, 1892). A very good discussion can be found in Ref. c13
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Such intersections are referred to as homoclinic intersections. This mechanism that originates chaos near a perturbed separatrix was discovered by Poincaré: see, e.g., H. Poincaré, Les Méthodes Nouvelles de la Mécanique Celeste (Gauthier-Villars, Paris, 1892). A very good discussion can be found in Ref. 13.
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24
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85037181271
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e-print quant-ph/9612037
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W. H. Zurek and J. P. Paz, e-print quant-ph/9612037.
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Zurek, W.H.1
Paz, J.P.2
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