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Phys. Rev. D 65, 083511 (2002) [9 pages]

Homoclinic chaos in the dynamics of a general Bianchi type-IX model

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H. P. de Oliveira*
NASA/Fermilab Astrophysics Center, Fermi National Accelerator Laboratory, Batavia, Illinois 60510-500
Universidade do Estado do Rio de Janeiro, Instituto de Física, Departamento de Física Teórica, CEP 20550-013 Rio de Janeiro, RJ, Brazil

A. M. Ozorio de Almeida
Centro Brasileiro de Pesquisas Físicas, Rua Dr. Xavier Sigaud, 150, CEP 22290-180, Rio de Janeiro, RJ, Brazil
Max Planck Institute for Physics of Complex Systems, Noethnitzer Strasse 38, 01187, Dresden, Germany

I. Damião Soares
Centro Brasileiro de Pesquisas Físicas, Rua Dr. Xavier Sigaud, 150, CEP 22290-180, Rio de Janeiro, RJ, Brazil

E. V. Tonini§
Centro Federal de Educação Tecnológica, CEFETES Avenida Vitória, 1729 Jucutuquara, CEP 29040-333, Vitória, ES, Brazil
Centro Brasileiro de Pesquisas Físicas, Rua Dr. Xavier Sigaud, 150, CEP 22290-180, Rio de Janeiro, RJ, Brazil

Received 31 August 2001; published 2 April 2002

The dynamics of a general Bianchi type-IX model with three scale factors is examined. The matter content of the model is assumed to be comoving dust plus a positive cosmological constant. The model presents a critical point of saddle-center-center type in the finite region of phase space. This critical point engenders in the phase space dynamics the topology of stable and unstable four dimensional tubes R×S3, where R is a saddle direction and S3 is the manifold of unstable periodic orbits in the center-center sector. A general characteristic of the dynamical flow is an oscillatory mode about orbits of an invariant plane of the dynamics which contains the critical point and a Friedmann-Robertson-Walker (FRW) singularity. We show that a pair of tubes (one stable, one unstable) emerging from the neighborhood of the critical point towards the FRW singularity have homoclinic transversal crossings. The homoclinic intersection manifold has topology R×S2 and is constituted of homoclinic orbits which are biasymptotic to the S3 center-center manifold. This is an invariant signature of chaos in the model, and produces chaotic sets in phase space. The model also presents an asymptotic de Sitter attractor at infinity and initial conditions sets are shown to have fractal basin boundaries connected to the escape into the de Sitter configuration (escape into inflation), characterizing the critical point as a chaotic scatterer.

© 2002 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.65.083511
DOI:
10.1103/PhysRevD.65.083511
PACS:
98.80.Hw, 04.25.Dm

*Electronic address: henrique@fnal.gov

Electronic address: ozorio@cbpf.br

Electronic address: ivano@cbpf.br

§Electronic address: tonini@etfes.br