We study the CP asymmetries in lepton number violating two body scattering processes and show explicitly how they vanish, in agreement with unitarity constraints. We relate these cross section asymmetries to the CP decay rate asymmetries of the intermediate massive neutrinos and show how the inclusion of the Universe expansion via Boltzmann equations is the key ingredient to allow the production of a non-vanishing asymmetry in spite of the unitarity constraint on the cross sections. We then show that the absorptive parts of both the one loop vertex and self energy corrections do contribute to the CP decay asymmetries
Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of...
We discuss the question of CP-violation in the effective Hamiltonian approach in models of leptogene...
Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmolo...
We study CP asymmetries in lepton-number violating two-body scattering processes and show how they a...
We study CP asymmetries in lepton-number violating two-body scattering processes and show how they a...
We work out the thermodynamic equations for the decays and scatterings of heavy Majorana neutrinos i...
We discuss how the cosmological baryon asymmetry can be achieved by the lepton family asymmetries of...
AbstractWe present an explicit computation of the CP asymmetry in scattering processes involving the...
Interactions of heavy Majorana neutrinos in the thermal phase of the early universe may be the origi...
We propose a new mechanism producing a non-vanishing lepton number asymmetry, based on decays of hea...
During the process of thermal leptogenesis temperature decreases by about one order of magnitude whi...
The mass term for Majorana neutrinos explicitly violates lepton number. Several authors have used th...
Neutrino oscillations, the evidence of dark matter and the baryon asymmetry in the universe can not ...
Both neutrinoless double beta decay and leptogenesis require neutrinos to be Majorana fermions. A r...
The biunitary parametrization of the neutrino Dirac mass matrix m(D) of the seesaw mechanism of neut...
Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of...
We discuss the question of CP-violation in the effective Hamiltonian approach in models of leptogene...
Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmolo...
We study CP asymmetries in lepton-number violating two-body scattering processes and show how they a...
We study CP asymmetries in lepton-number violating two-body scattering processes and show how they a...
We work out the thermodynamic equations for the decays and scatterings of heavy Majorana neutrinos i...
We discuss how the cosmological baryon asymmetry can be achieved by the lepton family asymmetries of...
AbstractWe present an explicit computation of the CP asymmetry in scattering processes involving the...
Interactions of heavy Majorana neutrinos in the thermal phase of the early universe may be the origi...
We propose a new mechanism producing a non-vanishing lepton number asymmetry, based on decays of hea...
During the process of thermal leptogenesis temperature decreases by about one order of magnitude whi...
The mass term for Majorana neutrinos explicitly violates lepton number. Several authors have used th...
Neutrino oscillations, the evidence of dark matter and the baryon asymmetry in the universe can not ...
Both neutrinoless double beta decay and leptogenesis require neutrinos to be Majorana fermions. A r...
The biunitary parametrization of the neutrino Dirac mass matrix m(D) of the seesaw mechanism of neut...
Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of...
We discuss the question of CP-violation in the effective Hamiltonian approach in models of leptogene...
Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmolo...