UV corrections in sgoldstino-less inflation
Entity
UAM. Departamento de Física TeóricaPublisher
Elsevier B.VDate
2016-05-25Citation
10.1016/j.physletb.2016.05.072
Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics 759 (2016): 121-125
ISSN
0370-2693 (print); 1873-2445 (online)DOI
10.1016/j.physletb.2016.05.072Funded by
The work of C.W. is supported by the ERC Advanced Grant SPLE under contract ERC-2012-ADG-20120216-320421, by the grant FPA2012-32828 from the MINECO, and by the grant SEV-2012-0249 of the “Centro de Excelencia Severo Ochoa” Programme. The work of L.H. is supported by the IISN and the Belgian Federal Science Policy through the Interuniversity Attraction Pole P7/37 “Fundamental Interactions”. The work of M.W. is supported by the SFB-Transregio TR33 “The Dark Universe” (Deutsche Forschungsgemeinschaft)Project
Gobierno de España. FPA2012-32828; Gobierno de España. SEV-2012-0249; info:eu-repo/grantAgreement/EC/FP7/320421Editor's Version
http://dx.doi.org/10.1016/j.physletb.2016.05.072Subjects
Physics; Sgoldstino; UV corrections; FísicaNote
Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UAMRights
© 2016 The AuthorsAbstract
We study the embedding of inflation with nilpotent multiplets in supergravity, in particular the decoupling of the sgoldstino scalar field. Instead of being imposed by hand, the nilpotency constraint on the goldstino multiplet arises in the low energy-effective theory by integrating out heavy degrees of freedom. We present explicit supergravity models in which a large but finite sgoldstino mass arises from Yukawa or gauge interactions. In both cases the inflaton potential receives two types of corrections. One is from the backreaction of the sgoldstino, the other from the heavy fields generating its mass. We show that these scale oppositely with the Volkov–Akulov cut-off scale, which makes a consistent decoupling of the sgoldstino nontrivial. Still, we identify a parameter window in which sgoldstino-less inflation can take place, up to corrections which flatten the inflaton potential
Files in this item
Google Scholar:Dudas, E.
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Heurtier, L.
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Wieck, C.
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Winkler, M.W.
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