dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-27T11:17:54Z
dc.date.accessioned2022-10-05T17:28:46Z
dc.date.available2014-05-27T11:17:54Z
dc.date.available2022-10-05T17:28:46Z
dc.date.created2014-05-27T11:17:54Z
dc.date.issued1993-12-01
dc.identifierNonlinearity, v. 6, n. 6, p. 973-995, 1993.
dc.identifier0951-7715
dc.identifierhttp://hdl.handle.net/11449/64417
dc.identifier10.1088/0951-7715/6/6/008
dc.identifierWOS:A1993MM78200008
dc.identifier2-s2.0-5644245016
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/3914477
dc.description.abstractThe Birkhoff-Gustavson normal form is employed to study separately chaos and resonances in a system with two degrees of freedom. In the integrable regime, tunnelling effects are appreciable when the nearest level spacings show oscillations. Tunnelling among states in the libration and rotation tori regions is also observed. The regularity of avoided crossings due to tunnelling indicates a collective effect and is associated with an isolated resonance. The spectral fluctuations also show a strong level correlation. The Husimi distribution, on the other hand, is insensitive to avoided crossings. An integrable approximation to the overlap of resonances is obtained and a theoretical description is given for an isolated cubic resonance plus a complex orbit. In the non-integrable regime chaos is stronger after overlapping and preferentially at low energies.
dc.languageeng
dc.relationNonlinearity
dc.relation1.926
dc.relation1,587
dc.rightsAcesso restrito
dc.sourceScopus
dc.titleClassical and quantal aspects of resonant normal forms
dc.typeArtigo


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