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Cosmic microwave background, matter–antimatter asymmetry and neutrino masses

2002/05/31 by W. Buchmüller, W. Buchmuller, Pasquale Di Bari +3 · 10 citations
Physics and Astronomy · #Astrophysics and Cosmic Phenomena #Neutrino Physics Research #Particle physics theoretical and experimental studies #astro-ph #hep-ph #hep-th

paper · pdf · doi:10.1016/s0550-3213(02)00737-x

published as Nucl.Phys.B643:367-390,2002; Erratum-ibid.B793:362,2008 · 28 pages, 14 figures included; v2: erratum added, M_1 lower bound in the strong wash-out regime (see Eq. (63)) relaxed by a factor 2/3

openalex publication_date 2002/11/01 · arxiv created 2007/08/10 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We study the implications of thermal leptogenesis for neutrino parameters. Assuming that decays of N1, the lightest of the heavy Majorana neutrinos, initiate baryogenesis, we show that the final baryon asymmetry is determined by only four parameters: the CP asymmetry epsilon1, the heavy neutrino mass M1, the effective light neutrino mass m1, and the quadratic mean m of the light neutrino masses. Imposing the CMB measurement of the baryon asymmetry as constraint on the neutrino parameters, we show, in a model independent way, that quasi-degenerate neutrinos are incompatible with thermal leptogenesis. For maximal CP asymmetry epsilon1, and neutrino masses in the range from (Δm2sol)1/2 to (Δm2atm)1/2, the baryogenesis temperature is TB = O(1010) GeV.

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