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`Little Higgs' models, in which the Higgs particle arises as a pseudo-Goldstone boson, have a natural mechanism of electroweak symmetry breaking associated with the large value of the top quark Yukawa coupling. The mechanism typically…

High Energy Physics - Phenomenology · Physics 2009-11-10 Maxim Perelstein , Michael E. Peskin , Aaron Pierce

If the gauge fields of the Standard Model propagate in TeV-size extra dimensions, they rapidly become strongly coupled and can form scalar bound states of quarks and leptons. If the quarks and leptons of the third generation propagate in 6…

High Energy Physics - Phenomenology · Physics 2014-11-17 Nima Arkani-Hamed , Hsin-Chia Cheng , Bogdan A. Dobrescu , Lawrence J. Hall

The recently reported observation of a new particle with mass about 125 GeV and couplings generally resembling those of the Standard Model Higgs boson provides a potential probe of the physics of electroweak symmetry breaking. Although the…

High Energy Physics - Phenomenology · Physics 2012-07-17 Andrew G. Cohen , Martin Schmaltz

The Abelian Higgs model forms an essential part of the electroweak standard model: it is the sector containing only Z and Higgs bosons. We present a diagram-based proof of the tree-level unitarity of this model inside the unitary gauge,…

High Energy Physics - Phenomenology · Physics 2018-01-17 Ronald Kleiss , Oscar Boher Luna

The LHC has been built to understand the dynamics at the origin of the breaking of the electroweak symmetry. Weakly coupled models with a fundamental Higgs boson have focused most of the attention of the experimental searches. We will…

High Energy Physics - Phenomenology · Physics 2015-06-04 J. R. Espinosa , C. Grojean , M. Muehlleitner

We have reconsidered theoretical upper bounds on the scalar boson masses within the two-Higgs-doublet model (THDM), employing the well-known technical condition of tree-level unitarity. Our treatment provides a modest extension and…

High Energy Physics - Phenomenology · Physics 2009-01-07 J. Horejsi , M. Kladiva

We present a realization of the idea that the Higgs boson is mainly a bound state of neutrinos induced by strong four-fermion interactions. The conflicts of this idea with the measured values of the top quark and Higgs boson masses are…

High Energy Physics - Phenomenology · Physics 2020-04-15 Leonardo Coito , Carlos Faubel , Arcadi Santamaria

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

We consider a model of dynamical electroweak symmetry breaking built on the idea of top-seesaw mechanism. The model features a fourth generation of vector-like QCD quarks responsible for the origin of the top-seesaw mechanism and leading to…

High Energy Physics - Phenomenology · Physics 2015-06-16 Hidenori S. Fukano , Kimmo Tuominen

We explore new physics scenarios which are optimally probed through precision Higgs measurements rather than direct collider searches. Such theories consist of additional electroweak charged or singlet states which couple directly to or mix…

High Energy Physics - Phenomenology · Physics 2015-06-12 Clifford Cheung , Samuel D. McDermott , Kathryn M. Zurek

We investigate the impact of electroweak (EW), scalar and QCD corrections to the full set of decay branching ratios of an additional CP-even Higgs boson ($H$) in the two Higgs doublet model with a softly broken $Z_2$ symmetry. We employ the…

High Energy Physics - Phenomenology · Physics 2022-08-10 Shinya Kanemura , Mariko Kikuchi , Kei Yagyu

Upper bounds for neutral as well as charged Higgs boson masses in a two-doublet model are obtained on the basis of tree unitarity conditions \`a la Lee, Quigg and Thacker. A wide variety of scattering processes are considered so extensively…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Kanemura , T. Kubota , E. Takasugi

We construct a calculable model of electroweak symmetry breaking in which the Higgs doublet emerges from the meta-stable SUSY breaking sector as a pseudo Nambu-Goldstone boson. The Higgs boson mass is further protected by the little Higgs…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yang Bai , JiJi Fan , Zhenyu Han

If the quadratic divergence of the standard electroweak model and its local variation with mass scale are both assumed to be zero, then a modified one-loop calculation yields m_t = 117 GeV and m_H = 183 GeV. Such a scenario may be the…

High Energy Physics - Phenomenology · Physics 2015-06-25 Ernest Ma

A heavy fourth generation with a mass of the order of 400 GeV or more could trigger dynamical electroweak symmetry breaking by forming condensates through the exchange of a fundamental Higgs scalar doublet. The dynamics leading to these…

High Energy Physics - Phenomenology · Physics 2015-05-20 P. Q. Hung , Chi Xiong

In a general supersymmetric standard model there is an upper bound $m_h$ on the tree level mass of the $CP=+1$ lightest Higgs boson which depends on the electroweak scale, $\tan \beta$ and the gauge and Yukawa couplings of the theory. When…

High Energy Physics - Phenomenology · Physics 2009-10-22 J. R. Espinosa , M. Quirós

We propose an alternative unification scenario where the Higgs self-coupling (lambda) is unified with the electroweak SU(2)L x U(1)Y interactions at an intermediate scale MGH, lower than the GUT scale. In this model the SM remains valid up…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Aranda , J. L. Diaz-Cruz , A. Rosado

We introduce a new class of Composite Higgs models in which electroweak symmetry is broken by a seesaw-like mechanism. If a global symmetry is broken sequentially at different scales, two sets of pseudo-Goldstone bosons will arise, one set…

High Energy Physics - Phenomenology · Physics 2016-01-27 Veronica Sanz , Jack Setford

Recently, a new class of models describing the quark mass hierarchy has been introduced. In this class, while the t quark plays a minor role in electroweak symmetry breaking (EWSB), it is crucial in providing the quark mass hierarchy. In…

High Energy Physics - Phenomenology · Physics 2010-04-29 Michio Hashimoto , V. A. Miransky

One of the simplest ways to account for the observed W-boson mass shift is to introduce the $SU(2)_L$ triplet Higgs boson with zero hypercharge, whose vacuum expectation value is about 3 GeV. If the triplet is heavy enough at…

High Energy Physics - Phenomenology · Physics 2023-01-19 Weikang Lin , Tsutomu T. Yanagida , Norimi Yokozaki
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