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September 24, 20252 citationsOpen Access

Alleviating the H₀ tension in Rastall gravity

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RMR. MohebiUniversity of KurdistanKGKh. Saaidi T. GolanbariUniversity of KurdistanKKK. KaramiUniversity of Kurdistan

Key Points

  • The Rastall ΛCDM model reduces the Hubble constant tension from local measurements to about 1.97σ to 2.18σ, showing promising adjustments.
  • Analysis used a comprehensive dataset including Big Bang Nucleosynthesis and Cosmic Microwave Background, ensuring robust parameter constraints.
  • Markov Chain Monte Carlo sampling was employed within a Bayesian statistical framework to estimate the model's parameters effectively.
  • Challenges remain with the σ8 parameter, indicating incomplete resolution of existing cosmic tensions for the Rastall model.

Abstract

The tension between measurements of the Hubble constant H₀ locally and the value inferred from Planck satellite have provided a strong motivation to explore theoretical frameworks beyond the standard cosmological model (ΛCDM). To this aim, we investigate the H₀ tension in the Rastall ΛCDM model (R-ΛCDM), formulated within the Rastall gravity framework as a phenomenological extension of General Relativity featuring a non-conserved energy-momentum tensor. To constrain the cosmological parameters, we employ a comprehensive combined dataset including Big Bang Nucleosynthesis (BBN), Hubble parameter H (z), Type Ia supernovae (SNe Ia), Baryon Acoustic Oscillations (BAO), Cosmic Microwave Background (CMB) anisotropies, and the growth rate of cosmic structures f (z) σ₈ (z). The estimation of model parameters is performed via Markov Chain Monte Carlo (MCMC) sampling within a Bayesian statistical framework. Our results show that the R-ΛCDM model, especially in closed geometry, reduces the H₀ tension, bringing the discrepancy with the local SH0ES measurements down to 1. 97σ to 2. 18σ. However, the tension related to the σ₈ parameter remains unresolved.

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Cite This Study

Mohebi et al. (2025) studied this question.

synapsesocial.com/papers/68d6d82e8b2b6861e4c3e2e7https://doi.org/10.48550/arxiv.2508.20129
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