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PreprintCC BY-NC-SA 4.0arXiv

Observational Constraints and Cosmic Growth Index of Realistic f(G) Gravity Frameworks using MCMC Analysis

Abstract

We present a comprehensive observational analysis of modified Gauss--Bonnet, or f(G), gravity by investigating both the background cosmological expansion and sub-horizon linear matter perturbations. We consider two viable functional forms: an arctangent parameterization (Model~I) and a generalized polynomial power-law model (Model~II). Using a Markov Chain Monte Carlo (MCMC) ensemble sampler, we constrain their parameter spaces through background and structure-growth observations. Our analysis employs cumulative combinations of Cosmic Chronometers (CC), the Pantheon+ Type Ia Supernovae compilation (PP), Redshift-Space Distortions (RSD), and the Year-1 Baryon Acoustic Oscillation measurements from the Dark Energy Spectroscopic Instrument (DESI BAO). The inclusion of DESI BAO data produces a noticeable downward shift in the preferred values of the Hubble constant, H0, and present matter density parameter, Ωm0. For Model~II, the full analysis yields H0=64.02+4.13*−3.08,km,s−1,Mpc−1 and Ω*m0=0.249+0.047−0.038. We further assess the statistical performance of the models relative to ΛCDM using ΔAICc, ΔBIC, and ΔDIC. For Model~II, the full dataset gives ΔAICc=4.233 and ΔDIC=5.971, favoring the ΛCDM baseline. At the perturbation level, both models exhibit stable growth histories compatible with large-scale structure observations. The models predict transitions in the late-time expansion dynamics at z≈0.5005 and z≈0.6086 for Models~I and II, respectively, highlighting differences in their cosmological evolution.

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BibTeX
@misc{dhankar2026observational,
  title = {{Observational Constraints and Cosmic Growth Index of Realistic $f(G)$ Gravity Frameworks using MCMC Analysis}},
  author = {Praveen Kumar Dhankar and Munyeshyaka Albert and Mohit Thakre and Joseph Ntahompagaze and Safiqul Islam and Farook Rahaman},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.16037},
  eprint = {2609.16037},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.16037},
  note = {CC BY-NC-SA 4.0},
}
RIS
TY  - UNPB
TI  - Observational Constraints and Cosmic Growth Index of Realistic f(G) Gravity Frameworks using MCMC Analysis
AU  - Praveen Kumar Dhankar
AU  - Munyeshyaka Albert
AU  - Mohit Thakre
AU  - Joseph Ntahompagaze
AU  - Safiqul Islam
AU  - Farook Rahaman
PY  - 2026
DA  - 2026/09/11
PB  - arXiv
DO  - 10.48550/arxiv.2609.16037
UR  - https://arxiv.org/abs/2609.16037
AB  - We present a comprehensive observational analysis of modified Gauss--Bonnet, or f(G), gravity by investigating both the background cosmological expansion and sub-horizon linear matter perturbations. We consider two viable functional forms: an arctangent parameterization (Model~I) and a generalized polynomial power-law model (Model~II). Using a Markov Chain Monte Carlo (MCMC) ensemble sampler, we constrain their parameter spaces through background and structure-growth observations. Our analysis employs cumulative combinations of Cosmic Chronometers (CC), the Pantheon+ Type Ia Supernovae compilation (PP), Redshift-Space Distortions (RSD), and the Year-1 Baryon Acoustic Oscillation measurements from the Dark Energy Spectroscopic Instrument (DESI BAO). The inclusion of DESI BAO data produces a noticeable downward shift in the preferred values of the Hubble constant, H_0, and present matter density parameter, Ω_m0. For Model~II, the full analysis yields H_0=64.02^+4.13*−3.08,km,s^−1,Mpc^−1 and Ω*m0=0.249^+0.047_−0.038. We further assess the statistical performance of the models relative to ΛCDM using ΔAIC_c, ΔBIC, and ΔDIC. For Model~II, the full dataset gives ΔAIC_c=4.233 and ΔDIC=5.971, favoring the ΛCDM baseline. At the perturbation level, both models exhibit stable growth histories compatible with large-scale structure observations. The models predict transitions in the late-time expansion dynamics at z≈0.5005 and z≈0.6086 for Models~I and II, respectively, highlighting differences in their cosmological evolution.
ER  -