L. Perivolaropoulos Department of Physics University of Ioannina Open page S. Fay, S. Nesseris, L.P. gr-qc/0703006.

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Presentation transcript:

L. Perivolaropoulos Department of Physics University of Ioannina Open page S. Fay, S. Nesseris, L.P. gr-qc/

Accelerating Cosmic Expansion Dark Energy (Quintessence, Perfect Fluid etc) Required Cosmic History: Cosmological Constant Modified Gravity ( f(R), Scalar-Tensor, BraneWorlds etc) 4 forms of f(R) (G.R. + 3) +1 form of f(R): Cosmic History H(z)Reconstruction of f(R) Dynamical System of Cosmic Evolution Modified Gravity (f(R), Scalar-Tensor, BraneWorlds etc) Carroll, Duvvuri, Trodden, Turner, astro-ph/ Amendola, Polarski, Tsujikawa, gr-qc/

Action: Generalized Friedman Equations Goal: Study the Dynamics Consistent with a LCDM Cosmic History: Flatness

New Variables: Constraint Equation: Dynamical System: Eliminate m assuming known x 3 Amendola et. al., gr-qc/

Dynamical System: Eliminate m(f(R)) assuming known x 3 Reduced Dynamical System: Find x 3 assuming a ΛCDM cosmic history:

Effective Equation of State: Cosmic Eras : x 3 values in each era:

Critical Point Definition: Stationary Dynamical Evolution Stability: has only negative eigenvalues Attractor attractor saddle unstable saddle unstable saddle attractor saddle attractor saddle unstable G.R.

Attractor Critical Points: Numerical Evolution confirms attractor behavior of critical points

Ω rad Ω DE ΩmΩm

ΩmΩm

Attractor General Relativity

Critical Point in each era (General Relativity)

1. Find F(N): 2. Find f(N): 3. Find R(N): Use numerically obtained 4. Reconstruct f(N) and f(R)

Required Cosmic History: 4 forms of f(R) (G.R. + 3) +1 form of f(R): Cosmic History H(z)Reconstruction of f(R) Dynamical System of Cosmic Evolution Nonlinear f(R) Theories can not mimick a ΛCDM Cosmology in a Consistent Manner