High Energy Physics - Phenomenology · arXiv:1311.2824 v1 · submitted 12 Nov 2013
Higgs Bosons in Extra Dimensions
The paper says
“The proximity of the singularity provides a strong wave-function renormalization for the Higgs field which suppresses the T and S parameters.”
from the abstract · picked out as the main claim by a classifier
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The paper
Abstract
In this paper, motivated by the recent discovery of a Higgs-like boson at the LHC with a mass m_H\simeq 126 GeV, we review different models where the hierarchy problem is solved by means of a warped extra dimension. In the Randall-Sundrum model electroweak observables provide very strong bounds on the mass of KK modes which motivates extensions to overcome this problem. Two extensions are briefly discussed. One particular extension is based on the deformation of the metric such that it strongly departs from the AdS_5 structure in the IR region while it goes asymptotically to AdS_5 in the UV brane. This model has the IR brane close to a naked metric singularity (which is outside the physical interval) characteristic of soft-walls constructions. The proximity of the singularity provides a strong wave-function renormalization for the Higgs field which suppresses the T and S parameters. The second class of considered extensions are based on the introduction of an extra gauge group in the bulk such that the custodial SU(2)_R symmetry is gauged and protects the T parameter. By further enlarging the bulk gauge symmetry one can find models where the Higgs is identified with the fifth component of gauge fields and for which the Higgs potential, along with the Higgs mass, can be dynamically determined by the Coleman-Weinberg mechanism.
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abstract compiled · 2026-09-23 · no language-model review
How the main claim is stated: asserted 1.00
What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.22 · human participants 0.01 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.48 · compares with prior results 0.29 · mentions code or data availability 0.02
The abstract, sentence by sentence
This table labels the abstract only (arXiv listing abstract v1). The number is the probability the classifier gave the label.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| In this paper, motivated by the recent discovery of a Higgs-like boson at the LHC with a mass m_H\simeq 126 GeV, we review different models where the hierarchy problem is solved by means of a warped extra dimension. | contribution 0.56 | 0.46 | 0.07 | asserted 0.89 |
| In the Randall-Sundrum model electroweak observables provide very strong bounds on the mass of KK modes which motivates extensions to overcome this problem. | background 0.96 | 0.06 | 0.04 | asserted 1.00 |
| Two extensions are briefly discussed. | contribution 0.92 | 0.49 | 0.02 | asserted 0.81 |
| One particular extension is based on the deformation of the metric such that it strongly departs from the AdS_5 structure in the IR region while it goes asymptotically to AdS_5 in the UV brane. | method 0.64 | 0.28 | 0.04 | asserted 1.00 |
| This model has the IR brane close to a naked metric singularity (which is outside the physical interval) characteristic of soft-walls constructions. | method 0.76 | 0.27 | 0.04 | asserted 1.00 |
| The proximity of the singularity provides a strong wave-function renormalization for the Higgs field which suppresses the T and S parameters. | interpretation 0.46 | 0.38 | 0.12 | asserted 1.00 |
| The second class of considered extensions are based on the introduction of an extra gauge group in the bulk such that the custodial SU(2)_R symmetry is gauged and protects the T parameter. | contribution 0.62 | 0.38 | 0.05 | asserted 0.99 |
| By further enlarging the bulk gauge symmetry one can find models where the Higgs is identified with the fifth component of gauge fields and for which the Higgs potential, along with the Higgs mass, can be dynamically determined by the Coleman-Weinberg mechanism. | contribution 0.69 | 0.42 | 0.11 | asserted 0.72 |
What kind of paper the classifier reports this is: review 1.00 · evidence from literature 0.79
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Not examined
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- references and citing sentences
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How the labels were made
Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,400 input tokens, $0.0003 reported.
Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON
Cited by 6 Pith papers
Reviewed papers on Pith that cite this one. The full citation record
- Cosmological Phase Transitions in Warped Space: Gravitational Waves and Collider Signatures hep-ph · Jun 2018
- Flavor Non-universal Pati-Salam Unification and Neutrino Masses hep-ph · Dec 2020
- A variant of 3-3-1 model for the generation of the SM fermion mass and mixing pattern hep-ph · May 2017
- Lepton-flavor universality violation in $R_K$ and $R_{D^{(*)}}$ from warped space hep-ph · Mar 2017
- $g_\mu-2$ from Vector-Like Leptons in Warped Space hep-ph · Jan 2017
- A Natural origin for the LHCb anomalies hep-ph · Aug 2016
How the literature uses it
13 arXiv papers cite this in 24 sentences
Papers citing it · 18 sentences without a confident label
Cites it as support 1 paper
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However, this same tuning will also be responsible for generating a light enough Higgs mode compared to the KK scale [ref] .
Unified Flavor Symmetry from warped dimensions · Introduction · 0.98
Cites it as background 5 papers
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We will not specify here the details of the five-dimensional (5D) model, as they were widely covered in the literature, Refs. [ref] , which we refer the reader to [For reviews see e.g. Refs. [ref] .].
Lepton-flavor universality violation in $R_K$ and $R_{D^{(*)}}$ from warped space · Introduction · 0.99
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In these theories, the back-reaction creates a naked singularity beyond the IR brane and they are dubbed soft-wall (SW) metric theories [ref] .
On Broad Kaluza-Klein Gluons · The model · 0.86
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Models with a bulk Higgs have been studied extensively after that, see Ref. [ref] .
Is the radion a bulk Higgs doublet? · Introduction · 0.99
What it cites · 20 sentences without a confident label
Uses data or values from 2 papers
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A useful fit relating the parameter $ρ$ with the mass of the first KK excitation $m_KK$ is given by Ref. [ref]
Warped Electroweak Breaking Without Custodial Symmetry · Standard Model in singular backgrounds · 0.84
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The calculation was done in Ref. [ref] with the result
Flavor Phenomenology in General 5D Warped Spaces · Electroweak precision observables · 0.86
Cites as support 2 papers
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As we will see in the next section (see also Refs. [ref] and [ref] ), a sizable $Z$ suppresses the $T$ ($S$) parameter by two (one) powers of $Z$, which leads to a corresponding reduction in the value of $ρ$ from EWPT.
Warped Electroweak Breaking Without Custodial Symmetry · Standard Model in Warped Extra Dimensions · 0.97
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As we will see in the next section (see also Refs. [ref] and [ref] ), a sizable $Z$ suppresses the $T$ ($S$) parameter by two (one) powers of $Z$, which leads to a corresponding reduction in the value of $ρ$ from EWPT.
Suppressing Electroweak Precision Observables in 5D Warped Models · Standard Model in Warped Extra Dimensions · 0.97
Cites as background 15 papers
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Constructions based on singular backgrounds are usually dubbed soft-walls [ref] .
Dynamical Soft-Wall AdS/QCD · Standard Model in singular backgrounds · 0.91
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Constructions based on singular backgrounds are usually dubbed soft-walls [ref] .
Linear Confinement and AdS/QCD · Standard Model in singular backgrounds · 0.91
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Constructions based on singular backgrounds are usually dubbed soft-walls [ref] .
Electroweak Breaking on a Soft Wall · Standard Model in singular backgrounds · 0.91
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