4.7 Article

Late-transition versus smooth H(z)-deformation models for the resolution of the Hubble crisis

期刊

PHYSICAL REVIEW D
卷 105, 期 6, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.105.063538

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资金

  1. FINEP
  2. FAPERJ
  3. European Union (ERDF) [5047222]
  4. Greece through Operational Program Competitiveness, Entrepreneurship and Innovation, NSRF 2014-2020
  5. CAPES
  6. Royal Society Dorothy Hodgkin Research Fellowship
  7. European Union (European Social Fund-ESF) through the Operational Programme Human Resources Development, Education and Lifelong Learning [MIS-5000432]
  8. CNPq (Brazil)
  9. FAPES (Brazil)
  10. European Union's Horizon 2020 research and innova-tion programme under the Marie Skodowska-Curie Grant [888258]
  11. Centro de Excelencia Severo Ochoa Program [SEV-2016-0597]
  12. Ramon y Cajal [RYC-2014-15843]
  13. COSMO/CBPF/MCTI
  14. [PGC2018-094773-B-C32]

向作者/读者索取更多资源

This study compares the fit quality of gravitational transition models to cosmological data with other smooth H(z) deformation models and the cosmological constant model. The results show that gravitational transition models have significant statistical advantages in addressing the Hubble crisis.
Gravitational transitions at low redshifts (z(t) < 0.1) have been recently proposed as a solution to the Hubble and growth tensions. Such transitions would naturally lead to a transition in the absolute magnitude M of type Ia supernovae (SNIa) at z(t )(late M transitions-LMT) and possibly in the dark energy equation of state parameter w (late w - M transitions). Here, we compare the quality of fit of this class of models to cosmological data, with the corresponding quality of fit of the cosmological constant model (ACDM) and some of the best smooth H(z) deformation models [wCDM (cold dark matter), Chevallier-Polarski-Linder, phenomenologically emergent dark energy]. We also perform model selection via the Akaike information criterion (AIC) and the Bayes factor. We use the full cosmic microwave background temperature anisotropy spectrum data, the baryon acoustic oscillations data, the Pantheon SNIa data, the SNIa absolute magnitude M as determined by Cepheid calibrators and the value of the Hubble constant H-0 as determined by local SNIa calibrated using Cepheids. We find that smooth H(z) deformation models perform worse than transition models for the following reasons: (1) they have a worse fit to low-z geometric probes (baryon acoustic oscillations and SNIa data); (2) they favor values of the SNIa absolute magnitude M that are lower as compared to the value M-c obtained with local Cepheid calibrators at z < 0.01; (3) They tend to worsen the Omega(m,0) - sigma(8,0) growth tension. We also find that the w - M transition model does not provide a better quality of fit to cosmological data than a pure M transition model (LMT), where w is fixed to the Lambda CDM value w = -1 at all redshifts. We conclude that the LMT model has significant statistical advantages over smooth late-time H(z) deformation models in addressing the Hubble crisis.

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