Abstract
We present a novel Affleck–Dine scenario for the generation of the observed baryon asymmetry of the Universe based on the non-trivial interplay between quintessential inflationary models containing a kinetic dominated post-inflationary era and a non-minimally coupled U(1) field with a weakly broken B−L symmetry. The non-minimal coupling to gravity renders heavy the Affleck–Dine field during inflation and avoids the generation of isocurvature fluctuations. During the subsequent kinetic era the Ricci scalar changes sign and the effective mass term of the Affleck–Dine field becomes tachyonic. This allows the field to dynamically acquire a large expectation value. The symmetry of the Affleck–Dine potential is automatically restored at the onset of radiation domination, when the Ricci scalar approximately equals zero. This inverse phase transition results in the coherent oscillation of the scalar field around the origin of its effective potential. The rotation of the displaced Affleck–Dine field in the complex plane generates a non-zero B−L asymmetry which can be eventually converted into a baryon asymmetry via the usual transfer mechanisms.
Highlights
One of the open issues in modern particle physics and cosmology is the origin of the observed matter-antimatter asymmetry of the Universe at temperatures below the MeV scale
The Standard Model of particle physics has in principle all the ingredients for generating a baryonic asymmetry during the electroweak phase transition [2], it cannot produce a sufficiently large baryon-toentropy ratio [3,4,5,6,7]
Quintessential inflation is a rather minimalistic paradigm involving a single degree of freedom, the cosmon, for explaining both the inflationary epoch and the dark energy dominated era
Summary
One of the open issues in modern particle physics and cosmology is the origin of the observed matter-antimatter asymmetry of the Universe at temperatures below the MeV scale. This asymmetry is traditionally quantified in terms of the so-called baryon-to-entropy ratio [1]. In contrast with the standard AD mechanism, the non-minimal coupling to gravity renders heavy the AD field during the inflationary epoch and confines it to the origin of its effective potential. This prevents the generation of sizable isocurvature perturbations.
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