- The paper calculates how MCPs contribute to dark radiation, affecting N_eff and the Universe’s thermal history.
- It uses CMB and BBN data to constrain MCP parameters, ruling out low masses (below 16 MeV) for sizeable minicharge values.
- The study establishes a framework for exploring hidden photon models, guiding future experimental and theoretical research beyond the Standard Model.
Overview of Dark Radiation Constraints on Minicharged Particles in Models with a Hidden Photon
The paper presented by Hendrik Vogel and Javier Redondo explores the cosmological implications of minicharged particles (MCPs) and hidden photons, an extension to the Standard Model with an unbroken hidden U(1) gauge symmetry. The primary objective is to calculate the thermalization and subsequent dark radiation contribution of these particles during the early Universe and its impact on Big Bang Nucleosynthesis (BBN) and Cosmic Microwave Background (CMB) anisotropies as measured by Planck.
Model Framework
The authors consider a hidden sector comprised of minicharged fermions with mass between 100 keV and 10 GeV, alongside massless hidden photons. MCPs acquire a small effective electric charge through kinetic mixing between the hidden photon and the hypercharge boson of the Standard Model, parameterized by ε. The paper explores a range of minicharges from 10−11 to 1, using a selection of hidden gauge couplings (g') to cover different potential physical scenarios.
Calculations and Constraints
The work provides a detailed thermal history of the Universe involving the hidden sector, accounting for interactions such as fermion pair annihilation and plasmon decay. The significant emphasis is laid on the effective number of relativistic species, Neff, a critical observable from the CMB data. The contribution of MCPs and hidden photons to Neff is calculated for varying MCP masses and minicharges.
The analysis reveals that MCPs can contribute significantly to dark radiation under certain parameters, leading to deviations in Neff from the expected value of 3.046, which includes contributions only from active neutrinos in the standard cosmological model. These deviations constrain MCP masses to be above the MeV scale for most values of ε and can reach up to GeV if ε approaches unity.
Another aspect explored is the impact on BBN, where the presence of additional relativistic energy density alters the expansion rate, potentially affecting the relic abundances of light nuclei, particularly He-4. Accurate calculations show consistency with constraints on Yp<0.263 to rule out MCPs with mf<16 MeV for minicharges larger than 1.4×10−8.
Implications and Future Directions
The constraints derived from the data of Planck and BBN significantly disfavour this class of particles with masses less than a GeV unless their minicharge is extremely small, thus narrowing the parameter space for MCPs substantially. This work provides a well-detailed map for future explorations and experimental verifications of hidden sectors and validates the utility of cosmological data in constraining subatomic physics beyond the Standard Model.
As future research develops, experimental bounds on MCPs could improve further, leading to more stringent constraints or potentially detecting such particles, assuming future CMB data continues to refine the precision on Neff. The paper also lays the groundwork for investigating other hidden sector models and their observational signatures, serving as a critical input for exploring physics at the interface of particle physics and cosmology.
This paper not only highlights the contribution of MCPs to the dark radiation but also sets an example of how comprehensive theoretical calculations coupled with precise experimental data can bridge insights into physics beyond the Standard Model and contribute to our understanding of the early Universe.