Positivity bounds on Minimal Flavor Violation

Abstract From general analyticity and unitarity requirements on the UV theory, positivity bounds on the Wilson coefficients of the dimension-8 operators composed of 4 fermions and two derivatives appearing in the Standard Model Effective Field Theory have been derived recently. We explore the fate o...

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Main Authors: Quentin Bonnefoy, Emanuele Gendy, Christophe Grojean
Format: Article
Language:English
Published: SpringerOpen 2021-04-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP04(2021)115
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spelling doaj-975eb05e21544b74ae09e78d9c22f6292021-04-18T11:06:54ZengSpringerOpenJournal of High Energy Physics1029-84792021-04-012021413310.1007/JHEP04(2021)115Positivity bounds on Minimal Flavor ViolationQuentin Bonnefoy0Emanuele Gendy1Christophe Grojean2Deutsches Elektronen-Synchrotron (DESY)Deutsches Elektronen-Synchrotron (DESY)Deutsches Elektronen-Synchrotron (DESY)Abstract From general analyticity and unitarity requirements on the UV theory, positivity bounds on the Wilson coefficients of the dimension-8 operators composed of 4 fermions and two derivatives appearing in the Standard Model Effective Field Theory have been derived recently. We explore the fate of these bounds in the context of models endowed with a Minimal Flavor Violation (MFV) structure, models in which the flavor structure of higher dimensional operators is inherited from the one already contained in the Yukawa sector of the Standard Model Lagrangian. Our goal is to check whether the general positivity bounds translate onto bounds on the Yukawa coefficients and/or on elements of the CKM matrix. MFV fixes the coefficients of dimension-8 operators up to some multiplicative flavor-blind factors and we find that, in the most generic setup, the freedom left by those unspecified coefficients is enough as not to constrain the parameters of the renormalizable Yukawa sector. On the contrary, the latter shape the allowed region for the former. Requiring said overall coefficients to take natural O 1 $$ \mathcal{O}(1) $$ values could give rise to bounds on the Yukawa couplings. Remarkably, at leading order in an expansion in powers of the Yukawa matrices, no bounds on the CKM entries can be retrieved.https://doi.org/10.1007/JHEP04(2021)115Beyond Standard ModelEffective Field Theories
collection DOAJ
language English
format Article
sources DOAJ
author Quentin Bonnefoy
Emanuele Gendy
Christophe Grojean
spellingShingle Quentin Bonnefoy
Emanuele Gendy
Christophe Grojean
Positivity bounds on Minimal Flavor Violation
Journal of High Energy Physics
Beyond Standard Model
Effective Field Theories
author_facet Quentin Bonnefoy
Emanuele Gendy
Christophe Grojean
author_sort Quentin Bonnefoy
title Positivity bounds on Minimal Flavor Violation
title_short Positivity bounds on Minimal Flavor Violation
title_full Positivity bounds on Minimal Flavor Violation
title_fullStr Positivity bounds on Minimal Flavor Violation
title_full_unstemmed Positivity bounds on Minimal Flavor Violation
title_sort positivity bounds on minimal flavor violation
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-04-01
description Abstract From general analyticity and unitarity requirements on the UV theory, positivity bounds on the Wilson coefficients of the dimension-8 operators composed of 4 fermions and two derivatives appearing in the Standard Model Effective Field Theory have been derived recently. We explore the fate of these bounds in the context of models endowed with a Minimal Flavor Violation (MFV) structure, models in which the flavor structure of higher dimensional operators is inherited from the one already contained in the Yukawa sector of the Standard Model Lagrangian. Our goal is to check whether the general positivity bounds translate onto bounds on the Yukawa coefficients and/or on elements of the CKM matrix. MFV fixes the coefficients of dimension-8 operators up to some multiplicative flavor-blind factors and we find that, in the most generic setup, the freedom left by those unspecified coefficients is enough as not to constrain the parameters of the renormalizable Yukawa sector. On the contrary, the latter shape the allowed region for the former. Requiring said overall coefficients to take natural O 1 $$ \mathcal{O}(1) $$ values could give rise to bounds on the Yukawa couplings. Remarkably, at leading order in an expansion in powers of the Yukawa matrices, no bounds on the CKM entries can be retrieved.
topic Beyond Standard Model
Effective Field Theories
url https://doi.org/10.1007/JHEP04(2021)115
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AT emanuelegendy positivityboundsonminimalflavorviolation
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