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Formalizing a unified dynamical system framework for f(R)f(R) and f(Q)f(Q) gravity

Published 21 Sep 2026 in gr-qc | (2609.24733v1)

Abstract: Going beyond the traditional Hubble-normalized framework, we formalize a unified dynamical system formulation for f(R)f(R) and coincident gauge f(Q)f(Q) gravity using three distinct sets of dimensionless variables: (1) kinematical cosmographic parameters, (2) the dark energy equation of state parameter ww (with its N=ln⁡aN=\ln a derivatives) and matter density abundance ΩmΩ_m, and (3) theory space parameters mi{m_i} characterizing the shape of the theory function. Our formulation is free of auxiliary variables, closing via three equivalent ways: (1) specifying a theory, (2) requiring a specific cosmological evolution, or (3) requiring a specific dark energy equation of state evolution. Each closure strategy is illustrated with explicit examples. The theory closure approach studies a case of Hu-Sawicki f(R)f(R) and f(Q)=−2Λ+Q+β−Qf(Q)=-2Λ+Q+β\sqrt{-Q} models, where traditional formalisms fail. A heteroclinic trajectory from a GR-matter-dominated epoch to a late-time de-Sitter epoch is general for f(Q)f(Q), but sensitive to initial conditions for f(R)f(R). The cosmographic and equation-of-state closure approaches compare f(R)f(R) and f(Q)f(Q) gravities kinematically equivalent to ΛΛCDM (j(z)=1j(z)=1) and dynamically equivalent to ΛΛCDM (w(z)=−1w(z)=-1). In both, GR acts as a cosmological past attractor for f(Q)f(Q) gravity, but not for f(R)f(R).

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