Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions

Spontaneous scale invariance breaking and the associated Goldstone boson, the dilaton, is investigated in renormalizable, unitary, interacting non-supersymmetric scalar field theories in $4-\varepsilon$ dimensions. At leading order it is possible to construct models which give rise...

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Main Author: Daniel Nogradi, Balint Ozsvath
Format: Article
Language:English
Published: SciPost 2022-05-01
Series:SciPost Physics
Online Access:https://scipost.org/SciPostPhys.12.5.169
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author Daniel Nogradi, Balint Ozsvath
author_facet Daniel Nogradi, Balint Ozsvath
author_sort Daniel Nogradi, Balint Ozsvath
collection DOAJ
description Spontaneous scale invariance breaking and the associated Goldstone boson, the dilaton, is investigated in renormalizable, unitary, interacting non-supersymmetric scalar field theories in $4-\varepsilon$ dimensions. At leading order it is possible to construct models which give rise to spontaneous scale invariance breaking classically and indeed a massless dilaton can be identified. Beyond leading order, in order to have no anomalous scale symmetry breaking in QFT, the models need to be defined at a Wilson-Fisher fixed point with exact conformal symmetry. It is shown that this requirement on the couplings is incompatible with having the type of flat direction which would be necessary for an exactly massless dilaton. As a result spontaneous scale symmetry breaking and an exactly massless dilaton can not occur in renormalizable, unitary $4-\varepsilon$ dimensional scalar QFT. The arguments apply to $\phi^6$ theory in $3-\varepsilon$ dimensions as well.
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spelling doaj.art-04c478ae48944d028db8b6041a8c91f42022-12-22T03:25:50ZengSciPostSciPost Physics2542-46532022-05-0112516910.21468/SciPostPhys.12.5.169Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensionsDaniel Nogradi, Balint OzsvathSpontaneous scale invariance breaking and the associated Goldstone boson, the dilaton, is investigated in renormalizable, unitary, interacting non-supersymmetric scalar field theories in $4-\varepsilon$ dimensions. At leading order it is possible to construct models which give rise to spontaneous scale invariance breaking classically and indeed a massless dilaton can be identified. Beyond leading order, in order to have no anomalous scale symmetry breaking in QFT, the models need to be defined at a Wilson-Fisher fixed point with exact conformal symmetry. It is shown that this requirement on the couplings is incompatible with having the type of flat direction which would be necessary for an exactly massless dilaton. As a result spontaneous scale symmetry breaking and an exactly massless dilaton can not occur in renormalizable, unitary $4-\varepsilon$ dimensional scalar QFT. The arguments apply to $\phi^6$ theory in $3-\varepsilon$ dimensions as well.https://scipost.org/SciPostPhys.12.5.169
spellingShingle Daniel Nogradi, Balint Ozsvath
Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
SciPost Physics
title Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
title_full Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
title_fullStr Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
title_full_unstemmed Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
title_short Dilaton in scalar QFT: a no-go theorem in 4-epsilon and 3-epsilon dimensions
title_sort dilaton in scalar qft a no go theorem in 4 epsilon and 3 epsilon dimensions
url https://scipost.org/SciPostPhys.12.5.169
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