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Related papers: Higgs and Top Quark Masses in the Standard Model w…

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Considering the standard model as an effective electroweak theory, in which we have no scalar mass term in the Higgs potential $(\mu^2=0)$, we show that the spontaneous symmetry breaking of $SU(2)_L \times U(1)$ can be induced by top loops.…

High Energy Physics - Phenomenology · Physics 2011-01-13 Thomas Hambye

We describe a deconstructed Higgsless model in which electroweak symmetry breaking results largely from a Higgsless mechanism while the top quark mass is generated by a topcolor mechanism. The top quark mass arises from a Yukawa coupling to…

High Energy Physics - Phenomenology · Physics 2010-09-15 R. Sekhar Chivukula , Neil D. Christensen , Baradhwaj Coleppa , Elizabeth H. Simmons

While the properties of the observed Higgs boson agree with the Standard Model predictions, the hierarchy of fermion masses lacks an explanation within the model. In this work, we propose a fresh approach to this problem, involving a…

High Energy Physics - Phenomenology · Physics 2024-02-22 S. Baek , J. Kersten , P. Ko , L. Velasco-Sevilla

Plausible interrelations between parameters of the standard model are studied. The empirical value of the top quark mass, when used in the renormalization group equations, suggests that the ratio of the colour SU(3) gauge coupling $g_3$,…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Ananthanarayan , J. Pasupathy

We study the implications for bounds on the top quark pole mass m_t in models with low scale supersymmetry following the discovery of the Standard Model-like Higgs boson. In the minimal supersymmetric standard model, we find that m_t >= 164…

High Energy Physics - Phenomenology · Physics 2015-06-18 Ilia Gogoladze , Rizwan Khalid , Shabbar Raza , Qaisar Shafi

We call attention to the fact that the gauge symmetry $SU(3)\times SU(2)_{_L}\times U(1)$ of the Standard Model can be easily and naturally extended by the local conformal symmetry connected with the possibility of choosing the local length…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marek Pawlowski , Ryszard Raczka , SINS/SISSA

The mass-generation mechanism is the most urgent problem of the modern particle physics. The discovery and study of the Higgs boson with the Large Hadron Collider at CERN are the highest priority steps to solve the problem. In this paper,…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. A. Bednyakov , N. D. Giokaris , A. V. Bednyakov

The Standard Model of particle physics contains about two dozen parameters - such as particle masses - whose origins are still unknown and cannot be predicted, but whose values are constrained through their interactions. In particular, the…

High Energy Physics - Experiment · Physics 2012-08-27 D0 Collaboration

We discuss a mechanism to generate hierarchy between masses of the top and bottom quarks without fine-tuning of the Yukawa coupling constants. In the framework of the two-Higgs-doublet model (THDM) with a discrete $Z_2$ symmetry, there…

High Energy Physics - Phenomenology · Physics 2011-02-28 Michio Hashimoto , Shinya Kanemura

Triviality and vacuum stability bounds on the Higgs and top quark masses in a rather general class of supersymmetric extensions of the Standard Model are compared with the corresponding bounds without supersymmetry. Due to generic…

High Energy Physics - Phenomenology · Physics 2009-10-22 U. Ellwanger , M. Lindner

Instead of right-handed neutrino singlets, the standard model is extended to include lepton triplets $(\Sigma^+, \Sigma^0, \Sigma^-)$. Each quark and lepton family may now transform under an anomaly-free $U(1)_X$ gauge symmetry, known…

High Energy Physics - Phenomenology · Physics 2021-03-17 Ernest Ma

A Lagrangian of electroweak interactions without Higgs is used to study the contributions of quarks and leptons to the masses of the W and the Z bosons. It is shown that the $SU(2)\times U(1)$ symmetry is broken by both fermion masses and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Bing An Li

It is studied that `no-scale' model makes hierarchy between scalar top mass and Z boson mass naturally. The supersymmetry breaking parameters are constrained by flavor changing neutral currents in minimal supersymmetric standard model. One…

High Energy Physics - Phenomenology · Physics 2016-09-06 Yuichi Chikira , Yukihiro Mimura

We propose a mechanism to generate hierarchy between masses of the top and bottom quarks without fine tuning of the Yukawa coupling constants in the context of the two Higgs doublet model (THDM). In the THDM with a discrete symmetry, there…

High Energy Physics - Phenomenology · Physics 2014-11-17 Michio Hashimoto , Shinya Kanemura

In the standard electroweak model, the measured top quark mass requires a sizeable Yukawa coupling to the fundamental scalar. This large coupling alone might induce a dynamical breaking of the electroweak symmetry as well as…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. Delepine , J. -M. Gerard , R. Gonzalez Felipe

`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

We show that if the Standard Model gauge fields and fermions propagate in extra dimenions, a composite Higgs field with the correct quantum number can arise naturally as a bound state due to the strong gauge interactions in higher…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hsin-Chia Cheng

In this article we propose a new strategy to address the Little Hierarchy problem. We show that the addition of a fourth generation with vector-like quarks to the minimal supersymmetric standard model (MSSM) can raise the predicted value of…

High Energy Physics - Phenomenology · Physics 2014-09-10 C. Faroughy , K. Grizzard

It is proposed to replace the Higgs boson of the standard model by a Lorentz- and gauge-invariant combination of SU(2) gauge bosons. A pair of Higgs bosons is identified with pairs of gauge bosons by setting their mass Lagrangians equal to…

High Energy Physics - Phenomenology · Physics 2015-11-18 F. J. Himpsel

We consider composite two-Higgs doublet models based on gauge-Yukawa theories with strongly interacting fermions generating the top-bottom mass hierarchy. The model features a single "universal" Higgs-Yukawa coupling, $ g $, which is…

High Energy Physics - Phenomenology · Physics 2020-05-27 Martin Rosenlyst , Christopher T. Hill
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