Cosmic Microwave Background, Matter-Antimatter Asymmetry and Neutrino Masses
| dc.creator | Buchmuller, W. | |
| dc.creator | Di Bari, P. | |
| dc.creator | Plumacher, M. | |
| dc.date | 2002-05-31 | |
| dc.date | 2007-08-10 | |
| dc.date.accessioned | 2026-07-07T11:31:15Z | |
| dc.date.available | 2026-07-07T11:31:15Z | |
| dc.description | We study the implications of thermal leptogenesis for neutrino parameters. Assuming that decays of N_1, 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 epsilon_1, the heavy neutrino mass M_1, the effective light neutrino mass \tilde{m}_1, and the quadratic mean \bar{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 epsilon_1, and neutrino masses in the range from (Δm^2_{sol})^{1/2} to (Δm^2_{atm})^{1/2}, the baryogenesis temperature is T_B = O(10^{10}) GeV. | |
| dc.description | 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 | |
| dc.identifier | https://arxiv.org/abs/hep-ph/0205349 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/0205349 | |
| dc.identifier | Nucl.Phys.B643:367-390,2002; Erratum-ibid.B793:362,2008 | |
| dc.identifier | doi:10.1016/S0550-3213(02)00737-X 10.1016/j.nuclphysb.2007.11.030 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/197205 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.subject | Astrophysics | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Cosmic Microwave Background, Matter-Antimatter Asymmetry and Neutrino Masses | |
| dc.type | text |