TY - JOUR
T1 - Kadanoff-Baym approach to flavour mixing and oscillations in resonant leptogenesis
AU - Bhupal Dev, P. S.
AU - Millington, Peter
AU - Pilaftsis, Apostolos
AU - Teresi, Daniele
N1 - Publisher Copyright:
© 2014 The Authors.
PY - 2015/2/1
Y1 - 2015/2/1
N2 - We describe a loopwise perturbative truncation scheme for quantum transport equations in the Kadanoff-Baym formalism, which does not necessitate the use of the so-called Kadanoff-Baym or quasi-particle ansaetze for dressed propagators. This truncation scheme is used to study flavour effects in the context of Resonant Leptogenesis (RL), showing explicitly that, in the weakly-resonant regime, there exist two distinct and pertinent flavour effects in the heavy-neutrino sector: (i) the resonant mixing and (ii) the oscillations between different heavy-neutrino flavours. Moreover, we illustrate that Kadanoff-Baym and quasi-particle ansaetze, whilst appropriate for the flavour-singlet dressed charged-lepton and Higgs propagators of the RL scenario, should not be applied to the dressed heavy-neutrino propagators. The use of these approximations for the latter is shown to capture only flavour oscillations, whilst discarding the separate phenomenon of flavour mixing.
AB - We describe a loopwise perturbative truncation scheme for quantum transport equations in the Kadanoff-Baym formalism, which does not necessitate the use of the so-called Kadanoff-Baym or quasi-particle ansaetze for dressed propagators. This truncation scheme is used to study flavour effects in the context of Resonant Leptogenesis (RL), showing explicitly that, in the weakly-resonant regime, there exist two distinct and pertinent flavour effects in the heavy-neutrino sector: (i) the resonant mixing and (ii) the oscillations between different heavy-neutrino flavours. Moreover, we illustrate that Kadanoff-Baym and quasi-particle ansaetze, whilst appropriate for the flavour-singlet dressed charged-lepton and Higgs propagators of the RL scenario, should not be applied to the dressed heavy-neutrino propagators. The use of these approximations for the latter is shown to capture only flavour oscillations, whilst discarding the separate phenomenon of flavour mixing.
UR - http://www.scopus.com/inward/record.url?scp=84918837942&partnerID=8YFLogxK
U2 - 10.1016/j.nuclphysb.2014.12.003
DO - 10.1016/j.nuclphysb.2014.12.003
M3 - Article
AN - SCOPUS:84918837942
SN - 0550-3213
VL - 891
SP - 128
EP - 158
JO - Nuclear Physics B
JF - Nuclear Physics B
ER -