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arXiv · 2507.05854

Addressing the Hubble Tension: Insights from Reversible and Irreversible Thermodynamic Processes

Abstract

We investigate reversible and irreversible thermodynamic processes in cosmology and their impact on the Hubble tension. Gravitationally induced adiabatic matter creation/annihilation is treated as irreversible, while energy exchange between the cosmic bulk and horizon is modeled as reversible. Two scenarios are proposed: Model I features matter creation/annihilation across all species with energy transfer to effective entropic dark energy; Model II considers dark matter creation/annihilation with energy flow from baryonic matter and radiation. The creation rate is parameterized as $\Gamma(t)=\Gamma_0 H$, with energy transfer controlled by $\gamma$. We constrain both models using Pantheon$+$ supernovae, CMB distance priors, baryon acoustic oscillations, gamma-ray bursts, and cosmic chronometers, with and without SH$_0$ES. When SH$_0$ES is included, matter annihilation ($\Gamma_0<0$) is statistically preferred, yielding $H_0 = 71.75 \pm 0.79$ km s$^{-1}$ Mpc$^{-1}$ (Model I) and $H_0 = 71.06 \pm 0.81$ km s$^{-1}$ Mpc$^{-1}$ (Model II), corresponding to $1.2\sigma$ and $1.8\sigma$ consistency with the SH$_0$ES value $73.17 \pm 0.86$ km s$^{-1}$ Mpc$^{-1}$. Matter creation ($\Gamma_0>0$) or pure energy flow ($\Gamma=0$) do not improve the tension. Without SH$_0$ES, information criteria show no preference over $\Lambda$CDM. For the matter annihilation/creation with energy flow, the effective entropic dark energy evolves dynamically, mimicking radiation and matter before recombination and approaching a cosmological constant at late times. These results demonstrate that thermodynamically motivated interactions can alleviate the Hubble tension when calibrated with local measurements, while remaining consistent with cosmological data.

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BibTeXRIS

Hussain Gohar. 2025-07-08. Addressing the Hubble Tension: Insights from Reversible and Irreversible Thermodynamic Processes. https://doi.org/10.1103/m4f8-4dj3

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