Baryogenesis, magnetogenesis and the strength of anomalous interactions

The production of the hypermagnetic gyrotropy is investigated under the assumption that the gauge coupling smoothly evolves during a quasi-de Sitter phase and then flattens out in the radiation epoch by always remaining perturbative. In the plane defined by the strength of the anomalous interactions and by the rate of evolution of the gauge coupling the actual weight of the pseudoscalar interactions turns out to be always rather modest if major deviations from the homogeneity are to be avoided during the inflationary phase. Even if the gauge power spectra are related by duality only in the absence of anomalous contributions, an approximate duality symmetry constrains the late-time form of the hypermagnetic power spectra. Since the hypermagnetic gyrotropy associated with the modes reentering prior to the phase transition must be released into fermions later on, the portions of the parameter space where the obtained baryon asymmetry is close to the observed value are the most relevant for the present ends. For the same range of parameters the magnetic power spectra associated with the modes reentering after symmetry breaking may even be of the order of a few hundredths of a nG over typical length scales comparable with the Mpc prior to the collapse of the protogalaxy.

Automated summary

The production of hypermagnetic gyrotropy is investigated under the assumption of smooth evolution of gauge coupling in a quasi-de Sitter phase, with the weight of pseudoscalar interactions being modest to avoid major deviations from homogeneity during inflationary phase. An approximate duality symmetry constrains the late-time form of hypermagnetic power spectra, with magnetic power spectra associated with modes reentering after symmetry breaking possibly reaching a few hundredths of a nG over typical length scales comparable to Mpc.