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A light Higgs scenario based on the TeV-scale supersymmetric strong dynamics
High Energy Physics - Phenomenology · Submitted 5 Jun 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Nevertheless, the SM-like Higgs boson is predicted to be as light as 125 GeV because these F-terms contribute to the mass of the SM-like Higgs boson not at the tree level but at the one-loop level.
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The abstract, sentence by sentence
We consider a model based on the supersymmetric QCD theory with N_c=2 and N_f=3. The theory is strongly coupled at the infrared scale \Lambda_H. Its low energy effective theory below \Lambda_H is described by the supersymmetric standard model with the Higgs sector that contains four iso-spin doublets, two neutral iso-spin singlets and two charged iso-spin singlets. If \Lambda_H is at the multi-TeV to 10 TeV, coupling constants for the F-terms of these composite fields are relatively large at the electroweak scale. Nevertheless, the SM-like Higgs boson is predicted to be as light as 125 GeV because these F-terms contribute to the mass of the SM-like Higgs boson not at the tree level but at the one-loop level. A large non-decoupling effect due to these F-terms appears in the one-loop correction to the triple Higgs boson coupling, which amounts to a few tens percent. Such a non-decoupling property in the Higgs potential realizes the strong first order phase transition, which is required for a successful scenario of electroweak baryogenesis.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider a model based on the supersymmetric QCD theory with N_c=2 and N_f=3. | contribution 0.61 | 0.57 | 0.03 | asserted 0.90 |
| s1 | The theory is strongly coupled at the infrared scale \Lambda_H. | background 0.48 | 0.23 | 0.03 | asserted 1.00 |
| s2 | Its low energy effective theory below \Lambda_H is described by the supersymmetric standard model with the Higgs sector that contains four iso-spin doublets, two neutral iso-spin singlets and two charged iso-spin singlets. | method 0.59 | 0.51 | 0.06 | asserted 1.00 |
| s3 | If \Lambda_H is at the multi-TeV to 10 TeV, coupling constants for the F-terms of these composite fields are relatively large at the electroweak scale. | result 0.84 | 0.64 | 0.05 | asserted 0.85 |
| s4 | Nevertheless, the SM-like Higgs boson is predicted to be as light as 125 GeV because these F-terms contribute to the mass of the SM-like Higgs boson not at the tree level but at the one-loop level. | result 0.99 | 0.81 | 0.54 | asserted 0.99 |
| s5 | A large non-decoupling effect due to these F-terms appears in the one-loop correction to the triple Higgs boson coupling, which amounts to a few tens percent. | result 1.00 | 0.82 | 0.13 | asserted 1.00 |
| s6 | Such a non-decoupling property in the Higgs potential realizes the strong first order phase transition, which is required for a successful scenario of electroweak baryogenesis. | interpretation 0.96 | 0.65 | 0.33 | asserted 0.99 |
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The paper
Original abstract
We consider a model based on the supersymmetric QCD theory with N_c=2 and N_f=3. The theory is strongly coupled at the infrared scale \Lambda_H. Its low energy effective theory below \Lambda_H is described by the supersymmetric standard model with the Higgs sector that contains four iso-spin doublets, two neutral iso-spin singlets and two charged iso-spin singlets. If \Lambda_H is at the multi-TeV to 10 TeV, coupling constants for the F-terms of these composite fields are relatively large at the electroweak scale. Nevertheless, the SM-like Higgs boson is predicted to be as light as 125 GeV because these F-terms contribute to the mass of the SM-like Higgs boson not at the tree level but at the one-loop level. A large non-decoupling effect due to these F-terms appears in the one-loop correction to the triple Higgs boson coupling, which amounts to a few tens percent. Such a non-decoupling property in the Higgs potential realizes the strong first order phase transition, which is required for a successful scenario of electroweak baryogenesis.
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How the literature uses it
2 arXiv papers cite this in 3 sentences
Papers citing it · 1 sentence without a confident label
Compares with it 1 paper
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Such large values of $μ_eff$ make this region of Fat Higgs/$λ$-SUSY parameter space slightly more unnatural than the low $tanβ$ region considered in Ref. [ref] .
A 125 GeV Fat Higgs at large $\tan \beta$ · Conclusions · 0.89
Cites it as background 1 paper
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Refs. [ref] have studied the phenomenological implications of models with such large $λ$ couplings, which we collectively call $λ$-SUSY models.
A 125 GeV Fat Higgs at large $\tan \beta$ · Introduction · 0.93
What it cites · 17 sentences without a confident label
Uses the method or tool of 1 paper
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Since we cannot determine the Kähler potential only from holomorphy, we take advantage of Na$ï$ve Dimensional Analysis (NDA) [ref] .
Naive Dimensional Analysis and Supersymmetry · Basic Framework · 0.99
Compares with 2 papers
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The effective theory has a similar structure to the “Four Higgs doublets and two charged singlets" (4HD$Ω$) model [ref] .
First-order electroweak phase transition powered by additional F-term loop effects in an extended supersymmetric Higgs sector · A Natural Model for the Light Higgs Boson from SUSY Strong Dynamics · 0.86
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At the first order of $v_u^2$ and $v_d^2$, the conditions (26) and (27) reduce to [equation] They give the same conditions for the electroweak symmetry breaking as in the Next-to-MSSM [ref] if we define the effective $Bμ$-term as [equation]
The Next-to-Minimal Supersymmetric Standard Model · Structure of the Effective Theory · 0.80
Cites as support 2 papers
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On the other hand, non-decoupling contributions of these fields in radiative corrections affect the triple Higgs boson coupling significantly [ref] , and can make the first order EWPT strong enough through the large F-term coupling constants [ref] .
Non-decoupling effects in supersymmetric Higgs sectors · Introduction · 0.99
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On the other hand, non-decoupling contributions of these fields in radiative corrections affect the triple Higgs boson coupling significantly [ref] , and can make the first order EWPT strong enough through the large F-term coupling constants [ref] .
First-order electroweak phase transition powered by additional F-term loop effects in an extended supersymmetric Higgs sector · Introduction · 0.99
Cites as background 2 papers
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In the decoupling limit, $m_h$ is given at the tree level by [ref] [equation] Here we introduce $tanβ≡v_u/v_d$ as usual.
The Next-to-Minimal Supersymmetric Standard Model · Structure of the Effective Theory · 0.85
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[ref] .) The most clear signatures of the model are events with two or three leptons and large missing transverse momentum.
Improved Naturalness with a Heavy Higgs: An Alternative Road to LHC Physics · Conclusions · 0.97
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