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Relaxing the Electroweak Scale: the Role of Broken dS Symmetry
Recently, a novel mechanism to address the hierarchy problem has been proposed \cite{Graham:2015cka}, where the hierarchy between weak scale physics and any putative `cutoff' $M$ is translated into a parametrically large field excursion for the so-called relaxion field, driving the Higgs mass t...
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Lenguaje: | eng |
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2015
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Acceso en línea: | https://dx.doi.org/10.1007/JHEP02(2016)077 http://cds.cern.ch/record/2039436 |
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author | Patil, Subodh P. Schwaller, Pedro |
author_facet | Patil, Subodh P. Schwaller, Pedro |
author_sort | Patil, Subodh P. |
collection | CERN |
description | Recently, a novel mechanism to address the hierarchy problem has been proposed \cite{Graham:2015cka}, where the hierarchy between weak scale physics and any putative `cutoff' $M$ is translated into a parametrically large field excursion for the so-called relaxion field, driving the Higgs mass to values much less than $M$ through cosmological dynamics. In its simplest incarnation, the relaxion mechanism requires nothing beyond the standard model other than an axion (the relaxion field) and an inflaton. In this note, we critically re-examine the requirements for successfully realizing the relaxion mechanism and point out that parametrically larger field excursions can be obtained for a given number of e-folds by simply requiring that the background break exact de Sitter invariance. We discuss several corollaries of this observation, including the interplay between the upper bound on the scale $M$ and the order parameter $\epsilon$ associated with the breaking of dS symmetry, and entertain the possibility that the relaxion could play the role of a curvaton. We find that a successful realization of the mechanism is possible with as few as $\mathcal O (10^3)$ e-foldings, albeit with a reduced cutoff $M \sim 10^6$ GeV for a dark QCD axion and outline a minimal scenario that can be made consistent with CMB observations. |
id | cern-2039436 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2015 |
record_format | invenio |
spelling | cern-20394362023-03-14T17:44:29Zdoi:10.1007/JHEP02(2016)077http://cds.cern.ch/record/2039436engPatil, Subodh P.Schwaller, PedroRelaxing the Electroweak Scale: the Role of Broken dS SymmetryParticle Physics - PhenomenologyRecently, a novel mechanism to address the hierarchy problem has been proposed \cite{Graham:2015cka}, where the hierarchy between weak scale physics and any putative `cutoff' $M$ is translated into a parametrically large field excursion for the so-called relaxion field, driving the Higgs mass to values much less than $M$ through cosmological dynamics. In its simplest incarnation, the relaxion mechanism requires nothing beyond the standard model other than an axion (the relaxion field) and an inflaton. In this note, we critically re-examine the requirements for successfully realizing the relaxion mechanism and point out that parametrically larger field excursions can be obtained for a given number of e-folds by simply requiring that the background break exact de Sitter invariance. We discuss several corollaries of this observation, including the interplay between the upper bound on the scale $M$ and the order parameter $\epsilon$ associated with the breaking of dS symmetry, and entertain the possibility that the relaxion could play the role of a curvaton. We find that a successful realization of the mechanism is possible with as few as $\mathcal O (10^3)$ e-foldings, albeit with a reduced cutoff $M \sim 10^6$ GeV for a dark QCD axion and outline a minimal scenario that can be made consistent with CMB observations.Recently, a novel mechanism to address the hierarchy problem has been proposed [1], where the hierarchy between weak scale physics and any putative ‘cutoff’ M is translated into a parametrically large field excursion for the so-called relaxion field, driving the Higgs mass to values much less than M through cosmological dynamics. In its simplest incarnation, the relaxion mechanism requires nothing beyond the standard model other than an axion (the relaxion field) and an inflaton. In this note, we critically re-examine the requirements for successfully realizing the relaxion mechanism and point out that parametrically larger field excursions can be obtained for a given number of e-folds by simply requiring that the background break exact de Sitter invariance. We discuss several corollaries of this observation, including the interplay between the upper bound on the scale M and the order parameter ϵ associated with the breaking of dS symmetry, and entertain the possibility that the relaxion could play the role of a curvaton. We find that a successful realization of the mechanism is possible with as few as $ \mathcal{O}\left(1{0}^3\right) $ e-foldings, albeit with a reduced cutoff M ∼ 10$^{6}$ GeV for a dark QCD axion and outline a minimal scenario that can be made consistent with CMB observations.Recently, a novel mechanism to address the hierarchy problem has been proposed \cite{Graham:2015cka}, where the hierarchy between weak scale physics and any putative `cutoff' $M$ is translated into a parametrically large field excursion for the so-called relaxion field, driving the Higgs mass to values much less than $M$ through cosmological dynamics. In its simplest incarnation, the relaxion mechanism requires nothing beyond the standard model other than an axion (the relaxion field) and an inflaton. In this note, we critically re-examine the requirements for successfully realizing the relaxion mechanism and point out that parametrically larger field excursions can be obtained for a given number of e-folds by simply requiring that the background break exact de Sitter invariance. We discuss several corollaries of this observation, including the interplay between the upper bound on the scale $M$ and the order parameter $\epsilon$ associated with the breaking of dS symmetry, and entertain the possibility that the relaxion could play the role of a curvaton. We find that a successful realization of the mechanism is possible with as few as $\mathcal O (10^3)$ e-foldings, albeit with a reduced cutoff $M \sim 10^6$ GeV for a dark QCD axion and outline a minimal scenario that can be made consistent with CMB observations.arXiv:1507.08649CERN-PH-TH-2015-179CERN-PH-TH-2015-179oai:cds.cern.ch:20394362015-07-30 |
spellingShingle | Particle Physics - Phenomenology Patil, Subodh P. Schwaller, Pedro Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title | Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title_full | Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title_fullStr | Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title_full_unstemmed | Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title_short | Relaxing the Electroweak Scale: the Role of Broken dS Symmetry |
title_sort | relaxing the electroweak scale: the role of broken ds symmetry |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP02(2016)077 http://cds.cern.ch/record/2039436 |
work_keys_str_mv | AT patilsubodhp relaxingtheelectroweakscaletheroleofbrokendssymmetry AT schwallerpedro relaxingtheelectroweakscaletheroleofbrokendssymmetry |