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Related papers: How light can the Higgs be?

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A modified criterion of the SM perturbative consistency is proposed. It is based on the analytic properties of the two-loop SM running couplings. Under the criterion adopted, the Higgs mass up to 380 GeV might not give rise to the strong…

High Energy Physics - Phenomenology · Physics 2009-11-07 Yu. F. Pirogov , O. V. Zenin

The current experimental lower bound on the Higgs mass significantly restricts the allowed parameter space in most realistic supersymmetric models, with the consequence that these models exhibit significant fine-tuning. We propose a…

High Energy Physics - Phenomenology · Physics 2014-11-17 Andreas Birkedal , Z. Chacko , Mary K. Gaillard

When the particle with mass $\sim 126$ GeV discovered at LHC is identified with the Higgs boson of the Standard Model, intriguing and challenging questions arise. Among them, the issue of the EW vacuum stability. We find that, despite…

High Energy Physics - Phenomenology · Physics 2015-06-16 Vincenzo Branchina , Emanuele Messina

The minimal supersymmetric standard model, and extensions, have stringent upper bounds on the mass of the lightest Higgs boson if perturbativity up to the Planck scale is assumed. We argue that these bounds are softened tremendously if the…

High Energy Physics - Phenomenology · Physics 2011-06-21 Puneet Batra , Antonio Delgado , David E. Kaplan , Tim M. P. Tait

The mass and the decay width of a Higgs boson in the minimal standard model are evaluated by a variational method in the limit of strong self-coupling interaction. The non-perturbative technique provides an interpolation scheme between…

High Energy Physics - Phenomenology · Physics 2010-12-17 Fabio Siringo

The neutral Higgs sector of the Minimal non Minimal Supersymmetric Standard Model is considered. By effective potential and R.G.E. supported method; an upper bound of the lightest Higgs is analysed. From the request of perturbativity of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Comelli

Inflation is nowadays a well-established paradigm consistent with all the observations. The precise nature of the inflaton is however unknown and its role could be played by any candidate able to imitate a scalar condensate in the slow-roll…

High Energy Physics - Phenomenology · Physics 2015-09-02 Javier Rubio

We consider the problem of a proper definition of the mass of a heavy unstable boson. It is shown how various definitions are related by the renormalization-scheme independence of the full resummed amplitude. This is made explicit for the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Wim Beenakker , Geert Jan van Oldenborgh , Jiri Hoogland , Ronald Kleiss

The parameters of the Higgs potential of the Minimal Supersymmetric Standard Model (MSSM) receive large radiative corrections which lift the mass of the lightest Higgs boson to the measured value of 126 GeV. Depending on the MSSM…

High Energy Physics - Phenomenology · Physics 2015-09-23 Markus Bobrowski , Guillaume Chalons , Wolfgang G. Hollik , Ulrich Nierste

The upper bound on the mass of the light CP-even Higgs boson of the minimal supersymmetric model (MSSM) depends on the supersymmetric particle spectrum via radiative loop effects. At present, complete one-loop results and partial two-loop…

High Energy Physics - Phenomenology · Physics 2007-05-23 Howard E. Haber

Extrapolating the Standard Model to high scales using the renormalisation group, three possibilities arise, depending on the mass of the Higgs boson: if the Higgs mass is large enough the Higgs self-coupling may blow up, entailing some new…

High Energy Physics - Phenomenology · Physics 2009-09-28 J. Ellis , J. R. Espinosa , G. F. Giudice , A. Hoecker , A. Riotto

The long-awaited Higgs particle H around 125 GeV has been observed at the LHC. Interpreting it as the standard model Higgs boson and if there is no new physics between electroweak and Planck scale, we then don't have a stable vacuum. Here,…

High Energy Physics - Phenomenology · Physics 2015-06-12 Yong Tang

The Higgs effective potential becomes unstable at approximately $10^{11}$ GeV, and if only standard model interactions are considered, the lifetime $\tau$ of the electroweak vacuum turns out to be much larger than the age of the Universe…

High Energy Physics - Phenomenology · Physics 2019-06-26 Vincenzo Branchina , Eloisa Bentivegna , Filippo Contino , Dario Zappalà

We consider the lightest Higgs boson in naturally R-parity conserving supersymmetric left-right models. We obtain an upper bound on the tree level mass of this lightest Higgs boson. This upper bound depends on the $SU(2)_L$ and $SU(2)_R$…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. Huitu , P. N. Pandita , K. Puolamäki

The current central experimental values of the parameters of the Standard Model give rise to a striking conclusion: metastability of the electroweak vacuum is favoured over absolute stability. A metastable vacuum for the Higgs boson implies…

Cosmology and Nongalactic Astrophysics · Physics 2019-01-21 Tommi Markkanen , Arttu Rajantie , Stephen Stopyra

In the Minimal Supersymmetric Standard Model (MSSM), a Higgs boson mass of 125 GeV can be obtained with moderately heavy scalar top superpartners provided they are highly mixed. The source of this mixing, a soft trilinear stop-stop-Higgs…

High Energy Physics - Phenomenology · Physics 2014-03-25 Nikita Blinov , David E. Morrissey

Within the Standard Model, the current Higgs and top quark data favor metastability of the electroweak vacuum, although the uncertainties are still significant. The true vacuum is many orders of magnitude deeper than ours and the barrier…

High Energy Physics - Phenomenology · Physics 2015-06-11 Oleg Lebedev , Alexander Westphal

We study the limits on the mass of the lightest Higgs in supersymmetric models extended with a gauge singlet when perturbative unification is required. We find that when maximum intermediate matter is added, the different evolution of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Masip , R. Munoz-Tapia

We compute the mass of the Higgs particle in a scheme in which SUSY is broken at a large scale M_{SS} well above the electroweak scale M_{EW}. Below M_{SS} one assumes one is just left with the SM with a fine-tuned Higgs potential. Under…

High Energy Physics - Phenomenology · Physics 2015-06-12 Luis E. Ibanez , Irene Valenzuela

In general electroweak models with weakly coupled (and otherwise arbitrary) Higgs sector there always exists in the spectrum a scalar state with mass controlled by the electroweak scale. A new and simple recipe to compute an analytical…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. Comelli , J. R. Espinosa
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