Systematic study of background cosmology in unitary Poincaré gauge theories with application to emergent dark radiation and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>H</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:math> tension
Will Barker, A. Lasenby, M. P. Hobson, Will Handley
Abstract
We propose a one-parameter extension to $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$, expected to strongly affect cosmological tensions. An effective dark radiation component in the early Universe redshifts away as hot dark matter, then quintessence, tracking the dominant equation-of-state parameter and leaving a falsifiable torsion field in the current epoch. This picture results from a new Poincar\'e gauge theory (PGT), one of the most promising among the latest batch of 58 PGTs found to be both power-counting renormalizable and free from ghosts and tachyons. We systematically categorize the cosmologies of 33 of these PGTs, as special cases of the most general parity-preserving, Ostrogradsky-stable PGT with a purely Yang-Mills action. The theory we consider contains two propagating massless gravitons, which may be ${J}^{P}={2}^{+}$ (long-range gravitation and gravitational waves). A conspiracy among the coupling constants eliminates the spatial curvature $k\ensuremath{\in}{\ifmmode\pm\else\textpm\fi{}1,0}$ from the field equations. We show that this ``$k$-screening'' is not restricted to conformal gravity theories. The flat Friedmann equations are then emergent, with potentially tension-resolving freedom at the early scale-invariant epoch that reliably gives way to an attractorlike state of modern $\mathrm{\ensuremath{\Lambda}}\mathrm{CDM}$ evolution. We compare with related theories and promising special cases, such as $k$-screened theories with negative-definite effective $k$, and more traditional theories with effective $\mathrm{\ensuremath{\Lambda}}$ and a ${J}^{P}={0}^{\ensuremath{-}}$ massive graviton (dark matter candidate). As a bonus, we analyze similarly constrained actions in the new extended Weyl gauge theory (eWGT). We show that in cosmology, PGT and eWGT span exactly the same classical phenomenology up to a linear map between their coupling constants, hinting at a deeper relationship between the two.