Axion effective potentials induced by heavy sterile fermions

Abstract A model of (3 + 1)-dimensional leptogenesis, proposed previously by the authors, requires a CPT Violating (CPTV) background of the Kalb–Ramond (KR) axion field. The KR axion is a pseudoscalar, which is dual to the field strength of the spin-one field present in the massless gravitational mu...

Full description

Bibliographic Details
Main Authors: Nick E. Mavromatos, Sarben Sarkar
Format: Article
Language:English
Published: SpringerOpen 2023-09-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-023-12049-x
_version_ 1797647168384794624
author Nick E. Mavromatos
Sarben Sarkar
author_facet Nick E. Mavromatos
Sarben Sarkar
author_sort Nick E. Mavromatos
collection DOAJ
description Abstract A model of (3 + 1)-dimensional leptogenesis, proposed previously by the authors, requires a CPT Violating (CPTV) background of the Kalb–Ramond (KR) axion field. The KR axion is a pseudoscalar, which is dual to the field strength of the spin-one field present in the massless gravitational multiplet in the theory of closed bosonic strings (compactified to four dimensions). Microscopic models for the emergence of such backgrounds are provided both by low-energy string-inspired gravitational theories with torsion (including (primordial) gravitational and axial gauge anomalies) and by Einstein–Cartan gravity, a closely related simpler model. In this work we examine the pseudoscalar quanta of the KR axion in this background using the methods of effective field theory. In our model for leptogenesis there is a single sterile right-handed neutrino (RHN) with mass $$m_N.$$ m N . At energies lower than $$m_N,$$ m N , an axion potential is derived by integrating out at one loop the sterile neutrino in the spirit of effective field theory. The stability of this axion potential is important for the viability of our model. The vacuum of this potential is generally metastable. The stability of the vacuum is determined by the ratio of the torsion-induced-axion coupling (which depends on the string mass scale) to $$m_N,$$ m N , which should be larger or equal to one, for the validity of our effective field theory. The vacuum is metastable only for axion couplings much larger than the sterile neutrino mass (large string mass scales, e.g. comparable to the four-dimensional Planck mass), with a lifetime much larger than the age of the observable Universe. By contrast, if axion couplings are comparable to the RHN mass the false vacuum is highly unstable, with a lifetime much smaller than the age of the observable Universe; in this case the CPTV leptogenesis scenario is not viable.
first_indexed 2024-03-11T15:12:28Z
format Article
id doaj.art-1d8fd2630a314b3c8c0cee3f782bc83c
institution Directory Open Access Journal
issn 1434-6052
language English
last_indexed 2024-03-11T15:12:28Z
publishDate 2023-09-01
publisher SpringerOpen
record_format Article
series European Physical Journal C: Particles and Fields
spelling doaj.art-1d8fd2630a314b3c8c0cee3f782bc83c2023-10-29T12:34:31ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522023-09-0183912110.1140/epjc/s10052-023-12049-xAxion effective potentials induced by heavy sterile fermionsNick E. Mavromatos0Sarben Sarkar1Physics Department, School of Applied Mathematical and Physical Sciences, National Technical University of AthensTheoretical Particle Physics and Cosmology Group, Department of Physics, King’s College LondonAbstract A model of (3 + 1)-dimensional leptogenesis, proposed previously by the authors, requires a CPT Violating (CPTV) background of the Kalb–Ramond (KR) axion field. The KR axion is a pseudoscalar, which is dual to the field strength of the spin-one field present in the massless gravitational multiplet in the theory of closed bosonic strings (compactified to four dimensions). Microscopic models for the emergence of such backgrounds are provided both by low-energy string-inspired gravitational theories with torsion (including (primordial) gravitational and axial gauge anomalies) and by Einstein–Cartan gravity, a closely related simpler model. In this work we examine the pseudoscalar quanta of the KR axion in this background using the methods of effective field theory. In our model for leptogenesis there is a single sterile right-handed neutrino (RHN) with mass $$m_N.$$ m N . At energies lower than $$m_N,$$ m N , an axion potential is derived by integrating out at one loop the sterile neutrino in the spirit of effective field theory. The stability of this axion potential is important for the viability of our model. The vacuum of this potential is generally metastable. The stability of the vacuum is determined by the ratio of the torsion-induced-axion coupling (which depends on the string mass scale) to $$m_N,$$ m N , which should be larger or equal to one, for the validity of our effective field theory. The vacuum is metastable only for axion couplings much larger than the sterile neutrino mass (large string mass scales, e.g. comparable to the four-dimensional Planck mass), with a lifetime much larger than the age of the observable Universe. By contrast, if axion couplings are comparable to the RHN mass the false vacuum is highly unstable, with a lifetime much smaller than the age of the observable Universe; in this case the CPTV leptogenesis scenario is not viable.https://doi.org/10.1140/epjc/s10052-023-12049-x
spellingShingle Nick E. Mavromatos
Sarben Sarkar
Axion effective potentials induced by heavy sterile fermions
European Physical Journal C: Particles and Fields
title Axion effective potentials induced by heavy sterile fermions
title_full Axion effective potentials induced by heavy sterile fermions
title_fullStr Axion effective potentials induced by heavy sterile fermions
title_full_unstemmed Axion effective potentials induced by heavy sterile fermions
title_short Axion effective potentials induced by heavy sterile fermions
title_sort axion effective potentials induced by heavy sterile fermions
url https://doi.org/10.1140/epjc/s10052-023-12049-x
work_keys_str_mv AT nickemavromatos axioneffectivepotentialsinducedbyheavysterilefermions
AT sarbensarkar axioneffectivepotentialsinducedbyheavysterilefermions