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Towards a precision calculation of the effective number of neutrinos N<sub>eff</sub> in the Standard Model. Part II. Neutrino decoupling in the presence of flavour oscillations and finite-temperature QED

Jack BennettSydney Consortium for Particle Physics and Cosmology, School of Physics, The University of New South Wales, Sydney NSW 2052, AustraliaGilles BuldgenCentre for Cosmology, Particle Physics and Phenomenology, Université Catholique de Louvain, Chemin du Cyclotron, 2, Louvain-la-Neuve B-1348, BelgiumP.F. de SalasThe Oskar Klein Centre for Cosmoparticle Physics, Department of Physics, Stockholm University, Roslagstullsbacken 21, Stockholm SE-106 91, SwedenMarco DrewesCentre for Cosmology, Particle Physics and Phenomenology, Université Catholique de Louvain, Chemin du Cyclotron, 2, Louvain-la-Neuve B-1348, BelgiumStefano GariazzoINFN, Sezione di Torino, Via P. Giuria 1, Torino I-10125, ItalyS. PastorInstituto de Física Corpuscular (CSIC-Universitat de València), Parc Científic UV, C/ Ca­te­drático José Beltrán, 2, Paterna, Valencia E-46980, SpainYvonne Y. Y. WongSydney Consortium for Particle Physics and Cosmology, School of Physics, The University of New South Wales, Sydney NSW 2052, Australia
2021en
ABI

Аннотация

Abstract We present in this work a new calculation of the standard-model benchmark value for the effective number of neutrinos, N eff SM , that quantifies the cosmological neutrino-to-photon energy densities. The calculation takes into account neutrino flavour oscillations, finite-temperature effects in the quantum electrodynamics plasma to O(e 3 ), where e is the elementary electric charge, and a full evaluation of the neutrino-neutrino collision integral. We provide furthermore a detailed assessment of the uncertainties in the benchmark N eff SM value, through testing the value's dependence on (i) optional approximate modelling of the weak collision integrals, (ii) measurement errors in the physical parameters of the weak sector, and (iii) numerical convergence, particularly in relation to momentum discretisation. Our new, recommended standard-model benchmark is N eff SM 3.0440 ±0.0002, where the nominal uncertainty is attributed predominantly to errors incurred in the numerical solution procedure (|δ N eff | ∼10 -4 ), augmented by measurement errors in the solar mixing angle sin 2θ 12 (|δ N eff | ∼10 -4 ).

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