Determining the Hubble constant without the sound horizon: A 3.6% constraint on H0 from galaxy surveys, CMB lensing, and supernovae

Oliver H. E. Philcox, Gerrit S. Farren, Blake D. Sherwin, Eric J. Baxter, and Dillon J. Brout
Phys. Rev. D 106, 063530 – Published 26 September 2022

Abstract

Many theoretical resolutions to the so-called “Hubble tension” rely on modifying the sound horizon at recombination, rs, and thus the acoustic scale used as a standard ruler in the cosmic microwave background (CMB) and large scale structure (LSS) datasets. As shown in a number of recent works, these observables can also be used to compute rs-independent constraints on H0 by making use of the horizon scale at matter-radiation equality, keq, which has different sensitivity to high redshift physics than rs. As such, rs- and keq-based measurements of H0 (within a ΛCDM framework) may differ if there is new physics present pre-recombination. In this work, we present the tightest constraints on the latter from current data, finding H0=64.82.5+2.2kms1Mpc1 at 68% CL from a combination of BOSS galaxy power spectra, Planck CMB lensing, and the newly released pantheon+ supernova constraints, as well as physical priors on the baryon density, neutrino mass, and spectral index. The BOSS and Planck measurements have different degeneracy directions, leading to the improved combined constraints, with a bound of H0=67.12.9+2.5 (63.63.6+2.9) from BOSS (Planck) alone in kms1Mpc1 units. The results show some dependence on the neutrino mass bounds, with the constraint broadening to H0=68.03.2+2.9kms1Mpc1 if we instead impose a weak prior on mν from terrestrial experiments rather than assuming mν<0.26eV, or shifting to H0=64.6±2.4kms1Mpc1 if the neutrino mass is fixed to its minimal value. Even without dependence on the sound horizon, our results are in 3σ tension with those obtained from the Cepheid-calibrated distance ladder, which begins to cause problems for new physics models that vary H0 by changing acoustic physics or the expansion history immediately prior to recombination.

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  • Received 11 April 2022
  • Accepted 13 September 2022

DOI:https://doi.org/10.1103/PhysRevD.106.063530

© 2022 American Physical Society

Physics Subject Headings (PhySH)

Gravitation, Cosmology & Astrophysics

Authors & Affiliations

Oliver H. E. Philcox1,2,3,4,*, Gerrit S. Farren5, Blake D. Sherwin5,6, Eric J. Baxter7, and Dillon J. Brout8

  • 1Center for Theoretical Physics, Department of Physics, Columbia University, New York, New York 10027, USA
  • 2Simons Society of Fellows, Simons Foundation, New York, New York 10010, USA
  • 3Department of Astrophysical Sciences, Princeton University, Princeton, New Jersey 08540, USA
  • 4School of Natural Sciences, Institute for Advanced Study, 1 Einstein Drive, Princeton, New Jersey 08540, USA
  • 5Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, United Kingdom
  • 6Kavli Institute for Cosmology, Institute of Astronomy, University of Cambridge, Cambridge CB3 0HA, United Kingdom
  • 7Institute for Astronomy, University of Hawai‘i, 2680 Woodlawn Drive, Honolulu, Hawaii 96822, USA
  • 8Center for Astrophysics—Harvard and Smithsonian, 60 Garden Street, Cambridge, Massachusetts 02138, USA

  • *ohep2@cantab.ac.uk

See Also

Determining the Hubble constant without the sound horizon: Perspectives with future galaxy surveys

Gerrit S. Farren, Oliver H. E. Philcox, and Blake D. Sherwin
Phys. Rev. D 105, 063503 (2022)

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Vol. 106, Iss. 6 — 15 September 2022

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