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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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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