Thermal Inflation with Flaton Chemical Potential

Show simple item record

dc.contributor.author Okada, Nobuchika
dc.date.accessioned 2019-05-14T17:49:37Z
dc.date.available 2019-05-14T17:49:37Z
dc.date.issued 2017-04-24 en_US
dc.identifier.uri http://ir.ua.edu/handle/123456789/5537
dc.description.abstract Thermal inflation driven by a scalar field called a “flaton” is a possible scenario to solve the cosmological moduli problem. We study a model of thermal inflation with a flaton chemical potential. In the presence of the chemical potential, a negative mass squared of the flaton—which is necessary to terminate thermal inflation—is naturally induced. We identify the allowed parameter region for the chemical potential (μ) and the flaton self-coupling constant to solve the cosmological moduli problem and satisfy theoretical consistencies. In general, the chemical potential is a free parameter and it can be taken to be much larger than the typical scale of soft supersymmetry-breaking parameters of O(1) TeV. For μ ≳ 10⁸ GeV, we find that the reheating temperature after thermal inflation can be high enough for the thermal leptogenesis scenario to be operative. This is in sharp contrast to the standard thermal inflation scenario, in which the reheating temperature is quite low and a special mechanism is necessary for generating a sufficient amount of baryon asymmetry in the Universe after thermal inflation. en_US
dc.format.mimetype application/pdf en_US
dc.language English en_US
dc.subject Baryogenesis & leptogenesis en_US
dc.subject Inflation en_US
dc.subject Gravitation, Cosmology & Astrophysics en_US
dc.title Thermal Inflation with Flaton Chemical Potential en_US
dc.type text en_US


Files in this item

This item appears in the following Collection(s)

Show simple item record

Search DSpace


Browse

My Account