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The Hubble Rate Trouble: An Effective Field Theory of Dark Matter

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arxiv 2212.13272 v1 pith:OMXCXZ25 submitted 2022-12-26 hep-ph gr-qchep-th

classification hep-phgr-qchep-th
keywords hubbleconstantdarkmattereffectiveleadmechanismparameter
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abstract

The Hubble constant inferred from the 6-parameter fit to the CMB power spectrum conflicts with the value obtained from direct measurements via type Ia supernova and Cepheids observations. We write down effective operators involving spin-0, spin-1/2, and spin-1 dark matter that lead to the relativistic production of dark matter particles at early times, and consequently lead to an increase in the number of relativistic degrees of freedom. This mechanism which is amenable to CMB, BBN, and structure formation observables can sufficiently raise the value of the Hubble constant derived from CMB and reconcile local and CMB probes of the Hubble constant. This mechanism alone increases $H_0$ up to $70\, {\rm km s^{-1} Mpc^{-1}}$, and with the help of a Phantom-like cosmology, reach $H_0 \simeq 71-73\, {\rm km s^{-1} Mpc^{-1}}$. Lastly, we outline the region of parameter space which reproduces $H_0 \simeq 71-73\, {\rm km s^{-1} Mpc^{-1}}$ while obeying all relevant constraints.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Interpreting the Hubble tension with a cascade decaying dark matter sector

    astro-ph.CO 2025-07 conditional novelty 6.0 of 10

    A cascade decaying dark matter model combining early and late effects still cannot reduce the Hubble tension below about 3 sigma, and is statistically disfavored relative to Lambda CDM.

  2. Updated BBN Bounds on Hadronic Injection in the Early Universe: The Gravitino Problem

    hep-ph 2025-01 conditional novelty 3.0 of 10

    With current light-element abundances, hadronic decays of long-lived particles are excluded above a yield curve in lifetime, and for gravitinos this translates into reheating temperature upper limits as low as 5×10^5 GeV.

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