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Volumn 57, Issue 2, 1998, Pages R1223-R1226

Chaos in effective classical and quantum dynamics

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Indexed keywords


EID: 0003236525     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.57.R1223     Document Type: Article
Times cited : (9)

References (27)
  • 1
    • 0003769394 scopus 로고
    • 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
    • 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).
    • (1991) Chaos and Quantum Physics
  • 2
    • 0003886232 scopus 로고
    • Cambridge University Press, Cambridge, G. Casati, B. V. Chirikov
    • Quantum Chaos: Between Order and Disorder, edited by G. Casati and B. V. Chirikov (Cambridge University Press, Cambridge, 1995).
    • (1995) Quantum Chaos: Between Order and Disorder
  • 3
    • 85037178575 scopus 로고    scopus 로고
    • O. Bohigas, in Ref. c1
    • O. Bohigas, in Ref. 1.
  • 5
    • 85037200317 scopus 로고    scopus 로고
    • M. V. Berry, in Ref. c1
    • M. V. Berry, in Ref. 1.
  • 13
    • 85037225120 scopus 로고    scopus 로고
    • e-print chao-dyn/9511007
    • T. C. Blum and H. T. Elze, e-print chao-dyn/9511007;
    • Blum, T.C.1    Elze, H.T.2
  • 16
    • 33744518241 scopus 로고
    • 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
    • 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);
    • (1961) J. Math. Phys. , vol.2 , pp. 407
    • Schwinger, J.1
  • 21
    • 0000254113 scopus 로고
    • 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
    • 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).
    • (1987) Rev. Mod. Phys. , vol.57 , pp. 617
    • Eckmann, J.-P.1    Ruelle, D.2
  • 22
    • 85037193458 scopus 로고    scopus 로고
    • The minimum of the classical potential energy has been fixed to zero for each value of [Formula Presented]
    • The minimum of the classical potential energy has been fixed to zero for each value of B.
  • 23
    • 85037199582 scopus 로고    scopus 로고
    • 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
    • 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.
  • 24
    • 85037181271 scopus 로고    scopus 로고
    • e-print quant-ph/9612037
    • W. H. Zurek and J. P. Paz, e-print quant-ph/9612037.
    • Zurek, W.H.1    Paz, J.P.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.