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The high energy fate of the minimal Goldstone Higgs
High Energy Physics - Phenomenology · Submitted 5 Jan 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that the model can remain stable and perturbative up to the Planck scale provided that the heavy beyond Standard Model scalar states have masses in a narrow interval around 3 TeV.
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The abstract, sentence by sentence
We consider a minimal model where the Higgs boson arises as an elementary pseudo-Nambu-Goldstone boson. The model is based on an extended scalar sector with global SO(5)/SO(4) symmetry. To achieve the correct electroweak symmetry breaking pattern, the model is augmented either with an explicit symmetry breaking term or an extra singlet scalar field. We consider separately both of these possibili- ties. We fit the model with the known particle spectrum at the electroweak scale and extrapolate to high energies using renormalization group. We find that the model can remain stable and perturbative up to the Planck scale provided that the heavy beyond Standard Model scalar states have masses in a narrow interval around 3 TeV.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider a minimal model where the Higgs boson arises as an elementary pseudo-Nambu-Goldstone boson. | contribution 0.84 | 0.52 | 0.03 | asserted 0.96 |
| s1 | The model is based on an extended scalar sector with global SO(5)/SO(4) symmetry. | method 0.64 | 0.35 | 0.02 | asserted 1.00 |
| s2 | To achieve the correct electroweak symmetry breaking pattern, the model is augmented either with an explicit symmetry breaking term or an extra singlet scalar field. | method 0.78 | 0.37 | 0.03 | asserted 0.96 |
| s3 | We consider separately both of these possibili- ties. | method 0.69 | 0.82 | 0.02 | asserted 0.76 |
| s4 | We fit the model with the known particle spectrum at the electroweak scale and extrapolate to high energies using renormalization group. | method 1.00 | 0.95 | 0.03 | asserted 0.95 |
| s5 | We find that the model can remain stable and perturbative up to the Planck scale provided that the heavy beyond Standard Model scalar states have masses in a narrow interval around 3 TeV. | result 1.00 | 0.96 | 0.92 | asserted 0.88 |
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Original abstract
We consider a minimal model where the Higgs boson arises as an elementary pseudo-Nambu-Goldstone boson. The model is based on an extended scalar sector with global SO(5)/SO(4) symmetry. To achieve the correct electroweak symmetry breaking pattern, the model is augmented either with an explicit symmetry breaking term or an extra singlet scalar field. We consider separately both of these possibili- ties. We fit the model with the known particle spectrum at the electroweak scale and extrapolate to high energies using renormalization group. We find that the model can remain stable and perturbative up to the Planck scale provided that the heavy beyond Standard Model scalar states have masses in a narrow interval around 3 TeV.
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What it cites · 15 sentences without a confident label
Cites as background 2 papers
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A possible interpretation of this discovery is to take the SM particle content (possibly extended by three right handed neutrinos [ref] ) to describe all elementary particle interactions below the Planck energy: with the observed Higgs mass the scalar self coupling does not develop a Landau pole and while the scalar self coupling runs negative around scale $10^10$ GeV, this results only in a metastability of the low energy vacuum [ref] .
Higgs mass and vacuum stability in the Standard Model at NNLO · Introduction · 0.89
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A possible interpretation of this discovery is to take the SM particle content (possibly extended by three right handed neutrinos [ref] ) to describe all elementary particle interactions below the Planck energy: with the observed Higgs mass the scalar self coupling does not develop a Landau pole and while the scalar self coupling runs negative around scale $10^10$ GeV, this results only in a metastability of the low energy vacuum [ref] .
Standard Model Vacuum Stability and Weyl Consistency Conditions · Introduction · 0.89
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