A note on the WGC, effective field theory and clockwork within string theory

Abstract It has been recently argued that Higgsing of theories with U(1) n gauge interactions consistent with the Weak Gravity Conjecture (WGC) may lead to effective field theories parametrically violating WGC constraints. The minimal examples typically involve Higgs scalars with a large charge with...

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Main Authors: Luis E. Ibáñez, Miguel Montero
Format: Article
Language:English
Published: SpringerOpen 2018-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2018)057
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spelling doaj-901744ea4ddb485d9a857a39a59f99802020-11-25T00:45:59ZengSpringerOpenJournal of High Energy Physics1029-84792018-02-012018211110.1007/JHEP02(2018)057A note on the WGC, effective field theory and clockwork within string theoryLuis E. Ibáñez0Miguel Montero1Departamento de Física Teórica and Instituto de Física Teórica UAM/CSIC, Universidad Autónoma de MadridInstitute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena, Utrecht UniversityAbstract It has been recently argued that Higgsing of theories with U(1) n gauge interactions consistent with the Weak Gravity Conjecture (WGC) may lead to effective field theories parametrically violating WGC constraints. The minimal examples typically involve Higgs scalars with a large charge with respect to a U(1) (e.g. charges (Z, 1) in U(1)2 with Z ≫ 1). This type of Higgs multiplets play also a key role in clockwork U(1) theories. We study these issues in the context of heterotic string theory and find that, even if there is no new physics at the standard magnetic WGC scale Λ ∼ g IR M P , the string scale is just slightly above, at a scale ∼kIRΛ $$ \sim \sqrt{k_{\mathrm{IR}}}\varLambda $$. Here k IR is the level of the IR U(1) worldsheet current. We show that, unlike the standard magnetic cutoff, this bound is insensitive to subsequent Higgsing. One may argue that this constraint gives rise to no bound at the effective field theory level since k IR is model dependent and in general unknown. However there is an additional constraint to be taken into account, which is that the Higgsing scalars with large charge Z should be part of the string massless spectrum, which becomes an upper bound k IR ≤ k 02, where k 0 is the level of the UV currents. Thus, for fixed k 0, Z cannot be made parametrically large. The upper bound on the charges Z leads to limitations on the size and structure of hierarchies in an iterated U(1) clockwork mechanism.http://link.springer.com/article/10.1007/JHEP02(2018)057Effective Field TheoriesSuperstrings and Heterotic StringsSpontaneous Symmetry Breaking
collection DOAJ
language English
format Article
sources DOAJ
author Luis E. Ibáñez
Miguel Montero
spellingShingle Luis E. Ibáñez
Miguel Montero
A note on the WGC, effective field theory and clockwork within string theory
Journal of High Energy Physics
Effective Field Theories
Superstrings and Heterotic Strings
Spontaneous Symmetry Breaking
author_facet Luis E. Ibáñez
Miguel Montero
author_sort Luis E. Ibáñez
title A note on the WGC, effective field theory and clockwork within string theory
title_short A note on the WGC, effective field theory and clockwork within string theory
title_full A note on the WGC, effective field theory and clockwork within string theory
title_fullStr A note on the WGC, effective field theory and clockwork within string theory
title_full_unstemmed A note on the WGC, effective field theory and clockwork within string theory
title_sort note on the wgc, effective field theory and clockwork within string theory
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-02-01
description Abstract It has been recently argued that Higgsing of theories with U(1) n gauge interactions consistent with the Weak Gravity Conjecture (WGC) may lead to effective field theories parametrically violating WGC constraints. The minimal examples typically involve Higgs scalars with a large charge with respect to a U(1) (e.g. charges (Z, 1) in U(1)2 with Z ≫ 1). This type of Higgs multiplets play also a key role in clockwork U(1) theories. We study these issues in the context of heterotic string theory and find that, even if there is no new physics at the standard magnetic WGC scale Λ ∼ g IR M P , the string scale is just slightly above, at a scale ∼kIRΛ $$ \sim \sqrt{k_{\mathrm{IR}}}\varLambda $$. Here k IR is the level of the IR U(1) worldsheet current. We show that, unlike the standard magnetic cutoff, this bound is insensitive to subsequent Higgsing. One may argue that this constraint gives rise to no bound at the effective field theory level since k IR is model dependent and in general unknown. However there is an additional constraint to be taken into account, which is that the Higgsing scalars with large charge Z should be part of the string massless spectrum, which becomes an upper bound k IR ≤ k 02, where k 0 is the level of the UV currents. Thus, for fixed k 0, Z cannot be made parametrically large. The upper bound on the charges Z leads to limitations on the size and structure of hierarchies in an iterated U(1) clockwork mechanism.
topic Effective Field Theories
Superstrings and Heterotic Strings
Spontaneous Symmetry Breaking
url http://link.springer.com/article/10.1007/JHEP02(2018)057
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