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Higgs-Yukawa model with higher dimension operators via extended mean field theory

Using Extended Mean Field Theory (EMFT) on the lattice, we study properties of the Higgs-Yukawa model as an approximation of the Standard Model Higgs sector, and the effect of higher dimension operators. We note that the discussion of vacuum stability is completely modified in the presence of a $\ph...

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Detalles Bibliográficos
Autores principales: Akerlund, Oscar, de Forcrand, Philippe
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.93.035015
http://cds.cern.ch/record/2048437
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author Akerlund, Oscar
de Forcrand, Philippe
author_facet Akerlund, Oscar
de Forcrand, Philippe
author_sort Akerlund, Oscar
collection CERN
description Using Extended Mean Field Theory (EMFT) on the lattice, we study properties of the Higgs-Yukawa model as an approximation of the Standard Model Higgs sector, and the effect of higher dimension operators. We note that the discussion of vacuum stability is completely modified in the presence of a $\phi^6$ term, and that the Higgs mass no longer appears fine tuned. We also study the finite temperature transition. Without higher dimension operators the transition is found to be second order (crossover with gauge fields) for the experimental value of the Higgs mass $M_h=125$ GeV. By taking a $\phi^6$ interaction in the Higgs potential as a proxy for a UV completion of the Standard Model, the transition becomes stronger and turns first order if the scale of new physics, i.e. the mass of the lightest mediator particle, is around $1.5$ TeV. This implies that electroweak baryogenesis may be viable in models which introduce new particles around that scale.
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spelling cern-20484372023-03-14T18:33:32Zdoi:10.1103/PhysRevD.93.035015http://cds.cern.ch/record/2048437engAkerlund, Oscarde Forcrand, PhilippeHiggs-Yukawa model with higher dimension operators via extended mean field theoryParticle Physics - LatticeUsing Extended Mean Field Theory (EMFT) on the lattice, we study properties of the Higgs-Yukawa model as an approximation of the Standard Model Higgs sector, and the effect of higher dimension operators. We note that the discussion of vacuum stability is completely modified in the presence of a $\phi^6$ term, and that the Higgs mass no longer appears fine tuned. We also study the finite temperature transition. Without higher dimension operators the transition is found to be second order (crossover with gauge fields) for the experimental value of the Higgs mass $M_h=125$ GeV. By taking a $\phi^6$ interaction in the Higgs potential as a proxy for a UV completion of the Standard Model, the transition becomes stronger and turns first order if the scale of new physics, i.e. the mass of the lightest mediator particle, is around $1.5$ TeV. This implies that electroweak baryogenesis may be viable in models which introduce new particles around that scale.Using extended mean field theory (EMFT) on the lattice, we study properties of the Higgs-Yukawa model as an approximation of the standard model Higgs sector, and the effect of higher dimension operators. We remark, as has been noted before, that the discussion of vacuum stability is completely modified in the presence of a ϕ6 term, and that the Higgs mass no longer appears fine tuned. We also study the finite temperature transition. Without higher dimension operators the transition is found to be second order (crossover with gauge fields) for the experimental value of the Higgs mass Mh=125  GeV. By taking a ϕ6 interaction in the Higgs potential as a proxy for a UV completion of the standard model, the transition becomes stronger and turns first order if the scale of new physics, i.e., the mass of the lightest mediator particle, is around 1.5 TeV. This implies that electroweak baryogenesis may be viable in models which introduce new particles around that scale.Using extended mean field theory (EMFT) on the lattice, we study properties of the Higgs-Yukawa model as an approximation of the standard model Higgs sector, and the effect of higher dimension operators. We note that the discussion of vacuum stability is completely modified in the presence of a $\phi^6$ term, and that the Higgs mass no longer appears fine tuned. We also study the finite temperature transition. Without higher dimension operators the transition is found to be second order (crossover with gauge fields) for the experimental value of the Higgs mass $M_h=125$ GeV. By taking a $\phi^6$ interaction in the Higgs potential as a proxy for a UV completion of the standard model, the transition becomes stronger and turns first order if the scale of new physics, i.e. the mass of the lightest mediator particle, is around $1.5$ TeV. This implies that electroweak baryogenesis may be viable in models which introduce new particles around that scale.arXiv:1508.07959CERN-PH-TH-2015-210NSF-KITP-15-123CERN-PH-TH-2015-210NSF-KITP-15-123oai:cds.cern.ch:20484372015-08-31
spellingShingle Particle Physics - Lattice
Akerlund, Oscar
de Forcrand, Philippe
Higgs-Yukawa model with higher dimension operators via extended mean field theory
title Higgs-Yukawa model with higher dimension operators via extended mean field theory
title_full Higgs-Yukawa model with higher dimension operators via extended mean field theory
title_fullStr Higgs-Yukawa model with higher dimension operators via extended mean field theory
title_full_unstemmed Higgs-Yukawa model with higher dimension operators via extended mean field theory
title_short Higgs-Yukawa model with higher dimension operators via extended mean field theory
title_sort higgs-yukawa model with higher dimension operators via extended mean field theory
topic Particle Physics - Lattice
url https://dx.doi.org/10.1103/PhysRevD.93.035015
http://cds.cern.ch/record/2048437
work_keys_str_mv AT akerlundoscar higgsyukawamodelwithhigherdimensionoperatorsviaextendedmeanfieldtheory
AT deforcrandphilippe higgsyukawamodelwithhigherdimensionoperatorsviaextendedmeanfieldtheory