2014/03/26 by Dario Buttazzo, Buttazzo, Dario
Computer Science · Physics and Astronomy · #Computational Physics and Python Applications #Cosmology and Gravitation Theories #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #Particle physics theoretical and experimental studies
paper · pdf · doi:10.48550/arxiv.1403.6535
openalex publication_date 2014/03/26 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The rather precise knowledge of the mass of the Higgs boson and of its couplings has important consequences for the physical phenomena taking place at the Fermi scale. We analyze some of these implications in the most motivated frameworks for physics at that energies - supersymmetry, models of a composite Higgs boson, and the Standard Model itself. At the same time, precision experiments in flavour physics require a highly non-generic structure of flavour and CP transitions. In any model of electroweak symmetry breaking with a relatively low scale of new phenomena, as motivated by naturalness, some mechanism has to be found in order to keep unwanted flavour effects under control. We devote particular attention to the consequences of the approximate U(2)3 symmetry exhibited by the quarks of the Standard Model. The combined analysis of the indirect constraints from flavour, Higgs and electroweak physics will allow us to outline a picture of some most natural models of physics near the Fermi scale. Although non trivially, a few models emerge that look capable of accommodating a 125 GeV Higgs boson, consistently with all the other constraints, with new particles in an interesting range for discovery at the LHC, as well as associated flavour signals. This is particularly interesting in view of the forthcoming improvements in the direct experimental investigation of that energies. Finally, the measurement of the last parameter of the Standard Model - the Higgs quartic coupling - has important consequences even if no new physics is present close to the Fermi scale: its near-critical value, which puts the electroweak vacuum in a metastable state close to a phase transition, may have an interesting connection with Planck-scale physics. We derive the bound for electroweak vacuum stability with full two-loop precision, and explore some possible implication of near-criticality.