A Kadanoff-Baym derivation yields Boltzmann equations with self-energy-corrected quasiparticle shells, adding a CP-violating velocity and force correction for fermions and none for bosons.
A different perspective on the vev insertion approximation for electroweak baryogenesis
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abstract
In the vev insertion approximation (VIA) the spacetime dependent part of the mass matrix is treated as a perturbation. We calculate the source terms for baryogenesis expanding both the self-energy and propagator to first order in mass insertions, which gives the same results as the usual approach of calculating the self-energy at second order and using zeroth order propagators. This procedure shows explicitly the equivalence between including the mass in the free or in the interaction Lagrangian. The VIA source then originates from the same term in the kinetic equation as the semi-classical source, but at leading order in the derivative expansion (the expansion in diamond operators). On top, another type of derivative expansion is done, which we estimate to be valid for a bubble width larger than the inverse thermal width. This cuts off the divergence in the VIA source in the limit that the thermal width vanishes.
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Systematic derivation of the Boltzmann equation for electroweak baryogenesis
A Kadanoff-Baym derivation yields Boltzmann equations with self-energy-corrected quasiparticle shells, adding a CP-violating velocity and force correction for fermions and none for bosons.