Criticality in the scale invariant standard model (squared)

We consider first the standard model Lagrangian with μh2 Higgs potential term set to zero. We point out that this classically scale invariant theory potentially exhibits radiative electroweak/scale symmetry breaking with very high vacuum expectation value (VEV) for the Higgs field, 〈ϕ〉≈1017–18 GeV....

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Main Authors: Robert Foot, Archil Kobakhidze, Alexander Spencer-Smith
Format: Article
Language:English
Published: Elsevier 2015-07-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269315004086
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spelling doaj-a1d574e31be3469f99be8a7c4b18cdb42020-11-25T00:35:47ZengElsevierPhysics Letters B0370-26931873-24452015-07-01747C16917210.1016/j.physletb.2015.05.064Criticality in the scale invariant standard model (squared)Robert Foot0Archil Kobakhidze1Alexander Spencer-Smith2ARC Centre of Excellence for Particle Physics at the Terascale, School of Physics, The University of Melbourne, VIC 3010, AustraliaARC Centre of Excellence for Particle Physics at the Terascale, School of Physics, The University of Sydney, NSW 2006, AustraliaARC Centre of Excellence for Particle Physics at the Terascale, School of Physics, The University of Sydney, NSW 2006, AustraliaWe consider first the standard model Lagrangian with μh2 Higgs potential term set to zero. We point out that this classically scale invariant theory potentially exhibits radiative electroweak/scale symmetry breaking with very high vacuum expectation value (VEV) for the Higgs field, 〈ϕ〉≈1017–18 GeV. Furthermore, if such a vacuum were realized then cancellation of vacuum energy automatically implies that this nontrivial vacuum is degenerate with the trivial unbroken vacuum. Such a theory would therefore be critical with the Higgs self-coupling and its beta function nearly vanishing at the symmetry breaking minimum, λ(μ=〈ϕ〉)≈βλ(μ=〈ϕ〉)≈0. A phenomenologically viable model that predicts this criticality property arises if we consider two copies of the standard model Lagrangian, with exact Z2 symmetry swapping each ordinary particle with a partner. The spontaneously broken vacuum can then arise where one sector gains the high scale VEV, while the other gains the electroweak scale VEV. The low scale VEV is perturbed away from zero due to a Higgs portal coupling, or via the usual small Higgs mass terms μh2, which softly break the scale invariance. In either case, the cancellation of vacuum energy requires Mt=(171.53±0.42) GeV, which is close to its measured value of (173.34±0.76) GeV.http://www.sciencedirect.com/science/article/pii/S0370269315004086
collection DOAJ
language English
format Article
sources DOAJ
author Robert Foot
Archil Kobakhidze
Alexander Spencer-Smith
spellingShingle Robert Foot
Archil Kobakhidze
Alexander Spencer-Smith
Criticality in the scale invariant standard model (squared)
Physics Letters B
author_facet Robert Foot
Archil Kobakhidze
Alexander Spencer-Smith
author_sort Robert Foot
title Criticality in the scale invariant standard model (squared)
title_short Criticality in the scale invariant standard model (squared)
title_full Criticality in the scale invariant standard model (squared)
title_fullStr Criticality in the scale invariant standard model (squared)
title_full_unstemmed Criticality in the scale invariant standard model (squared)
title_sort criticality in the scale invariant standard model (squared)
publisher Elsevier
series Physics Letters B
issn 0370-2693
1873-2445
publishDate 2015-07-01
description We consider first the standard model Lagrangian with μh2 Higgs potential term set to zero. We point out that this classically scale invariant theory potentially exhibits radiative electroweak/scale symmetry breaking with very high vacuum expectation value (VEV) for the Higgs field, 〈ϕ〉≈1017–18 GeV. Furthermore, if such a vacuum were realized then cancellation of vacuum energy automatically implies that this nontrivial vacuum is degenerate with the trivial unbroken vacuum. Such a theory would therefore be critical with the Higgs self-coupling and its beta function nearly vanishing at the symmetry breaking minimum, λ(μ=〈ϕ〉)≈βλ(μ=〈ϕ〉)≈0. A phenomenologically viable model that predicts this criticality property arises if we consider two copies of the standard model Lagrangian, with exact Z2 symmetry swapping each ordinary particle with a partner. The spontaneously broken vacuum can then arise where one sector gains the high scale VEV, while the other gains the electroweak scale VEV. The low scale VEV is perturbed away from zero due to a Higgs portal coupling, or via the usual small Higgs mass terms μh2, which softly break the scale invariance. In either case, the cancellation of vacuum energy requires Mt=(171.53±0.42) GeV, which is close to its measured value of (173.34±0.76) GeV.
url http://www.sciencedirect.com/science/article/pii/S0370269315004086
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