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Finite Theories after the discovery of a Higgs-like boson at the LHC

Finite Unified Theories (FUTs) are N = 1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. Confronting the predictions of SU(5) FUTs with the top and bo...

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Autores principales: Heinemeyer, Sven, Mondragon, Myriam, Zoupanos, George
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2012.12.042
http://cds.cern.ch/record/1494874
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author Heinemeyer, Sven
Mondragon, Myriam
Zoupanos, George
author_facet Heinemeyer, Sven
Mondragon, Myriam
Zoupanos, George
author_sort Heinemeyer, Sven
collection CERN
description Finite Unified Theories (FUTs) are N = 1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. Confronting the predictions of SU(5) FUTs with the top and bottom quark masses and other low-energy experimental constraints a light Higgs-boson mass in the range M_h ~ 121-126 GeV was predicted, in striking agreement with the recent discovery of a Higgs-like state around ~ 125.7 GeV at ATLAS and CMS. Furthermore the favoured model, a finiteness constrained version of the MSSM, naturally predicts a relatively heavy spectrum with coloured supersymmetric particles above ~ 1.5 TeV, consistent with the non-observation of those particles at the LHC. Restricting further the best FUT's parameter space according to the discovery of a Higgs-like state and B-physics observables we find predictions for the rest of the Higgs masses and the s-spectrum.
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spelling cern-14948742023-03-14T17:54:55Zdoi:10.1016/j.physletb.2012.12.042http://cds.cern.ch/record/1494874engHeinemeyer, SvenMondragon, MyriamZoupanos, GeorgeFinite Theories after the discovery of a Higgs-like boson at the LHCParticle Physics - PhenomenologyFinite Unified Theories (FUTs) are N = 1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. Confronting the predictions of SU(5) FUTs with the top and bottom quark masses and other low-energy experimental constraints a light Higgs-boson mass in the range M_h ~ 121-126 GeV was predicted, in striking agreement with the recent discovery of a Higgs-like state around ~ 125.7 GeV at ATLAS and CMS. Furthermore the favoured model, a finiteness constrained version of the MSSM, naturally predicts a relatively heavy spectrum with coloured supersymmetric particles above ~ 1.5 TeV, consistent with the non-observation of those particles at the LHC. Restricting further the best FUT's parameter space according to the discovery of a Higgs-like state and B-physics observables we find predictions for the rest of the Higgs masses and the s-spectrum.Finite Unified Theories (FUTs) are N=1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. Confronting the predictions of SU(5) FUTs with the top and bottom quark masses and other low-energy experimental constraints a light Higgs boson mass in the range Mh∼121–126 GeV was predicted, in striking agreement with the recent discovery of a Higgs-like state around ∼125.7 GeV at ATLAS and CMS. Furthermore the favoured model, a finiteness constrained version of the MSSM, naturally predicts a relatively heavy spectrum with coloured supersymmetric particles above ∼1.5 TeV , consistent with the non-observation of those particles at the LHC. Restricting further the best FUTʼs parameter space according to the discovery of a Higgs-like state and B -physics observables we find predictions for the rest of the Higgs masses and the s-spectrum.Finite Unified Theories (FUTs) are N = 1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. Confronting the predictions of SU(5) FUTs with the top and bottom quark masses and other low-energy experimental constraints a light Higgs-boson mass in the range M_h ~ 121-126 GeV was predicted, in striking agreement with the recent discovery of a Higgs-like state around ~ 125.7 GeV at ATLAS and CMS. Furthermore the favoured model, a finiteness constrained version of the MSSM, naturally predicts a relatively heavy spectrum with coloured supersymmetric particles above ~ 1.5 TeV, consistent with the non-observation of those particles at the LHC. Restricting further the best FUT's parameter space according to the discovery of a Higgs-like state and B-physics observables we find predictions for the rest of the Higgs masses and the s-spectrum.arXiv:1211.3765CERN-PH-TH-2012-217CERN-PH-TH-2012-217oai:cds.cern.ch:14948742012-11-19
spellingShingle Particle Physics - Phenomenology
Heinemeyer, Sven
Mondragon, Myriam
Zoupanos, George
Finite Theories after the discovery of a Higgs-like boson at the LHC
title Finite Theories after the discovery of a Higgs-like boson at the LHC
title_full Finite Theories after the discovery of a Higgs-like boson at the LHC
title_fullStr Finite Theories after the discovery of a Higgs-like boson at the LHC
title_full_unstemmed Finite Theories after the discovery of a Higgs-like boson at the LHC
title_short Finite Theories after the discovery of a Higgs-like boson at the LHC
title_sort finite theories after the discovery of a higgs-like boson at the lhc
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2012.12.042
http://cds.cern.ch/record/1494874
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