The promising future of a robust cosmological neutrino mass measurement
Thejs Brinckmann, Deanna C. Hooper, Maria Archidiacono, Julien Lesgourgues, Tim Sprenger
TL;DR
This work forecasts how well future cosmological data can constrain the total neutrino mass $M_ u$ across a grid of cosmological models and experimental configurations. Using MCMC forecasts with mock likelihoods implemented in MontePython-CLASS, and conservatively excluding non-linear scale information, the authors compare 35 combinations of CMB and LSS data, including LiteBIRD, CORE-M5, CMB-S4, and PICO with DESI, Euclid, and SKA. In the minimal $oldsymbol{ ext{ΛCDM}}+M_ u$ setup, several combinations yield high-significance detections of $M_ u$ around $0.06$ eV, and including a precise $ au_{ ext{reio}}$ prior from 21 cm measurements can boost sensitivity substantially; extending to $N_{ ext{eff}}$, $w_0$, and $w_a$ introduces degeneracies that reduce, but do not erase, the neutrino mass constraints, with $N_{ ext{eff}}$ constraints benefiting especially from CMB-S4 and Euclid. The paper emphasizes the powerful complementarity of CMB and LSS data, provides a framework for comparing future experiments on neutrino mass sensitivity, and discusses caveats related to foregrounds and non-linear modeling that could affect real-data outcomes.
Abstract
We forecast the sensitivity of thirty-five different combinations of future Cosmic Microwave Background and Large Scale Structure data sets to cosmological parameters and to the total neutrino mass. We work under conservative assumptions accounting for uncertainties in the modelling of systematics. In particular, for galaxy redshift surveys, we remove the information coming from non-linear scales. We use Bayesian parameter extraction from mock likelihoods to avoid Fisher matrix uncertainties. Our grid of results allows for a direct comparison between the sensitivity of different data sets. We find that future surveys will measure the neutrino mass with high significance and will not be substantially affected by potential parameter degeneracies between neutrino masses, the density of relativistic relics, and a possible time-varying equation of state of Dark Energy.
