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Related papers: Constituent Quark Masses and the Electroweak Stand…

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The weak bosons consist of two fermions, bound by a new confining gauge force. The mass scale of this new interaction is determined. At energies below 0.5 TeV the standard electroweak theory is valid. A neutral isoscalar weak boson X must…

High Energy Physics - Phenomenology · Physics 2015-05-28 Harald Fritzsch

Exact low energy expressions are derived for the top-squark and higgs masses, taking into account radiative contributions due to a heavy top quark. Their masses are expressed as analytic functions of $m_{1/2}$, $m_{3/2}$, $m_t$ and…

High Energy Physics - Phenomenology · Physics 2009-10-22 G. K. Leontaris

Within composite Higgs models based on the top seesaw mechanism, we show that the Higgs field can arise as the pseudo Nambu-Goldstone boson of the broken U(3)_L chiral symmetry associated with a vector-like quark and the t-b doublet. As a…

High Energy Physics - Phenomenology · Physics 2015-06-18 Hsin-Chia Cheng , Bogdan A. Dobrescu , Jiayin Gu

Recent experimental improvements on K-decay data allow for a precise extraction of the strangeness-changing scalar K pi form factor and the related strange scalar spectral function. On the basis of this scalar as well as the corresponding…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Jamin , J. A. Oller , A. Pich

We investigate the neutron to proton decay via a Higgs mechanism in the framework of a reinterpreted Kogut-Susskind Hamiltonian on the Lie group u(3). We calculate expressions for a scalar Higgs mass, an electroweak energy scale, and vector…

High Energy Physics - Phenomenology · Physics 2014-05-02 Ole L. Trinhammer

We study constraints on Composite Higgs models with fermion partial compositeness from electroweak precision measurements, including the 2022 $W$-boson mass result from the CDF collaboration. We focus on models where the Composite Higgs…

High Energy Physics - Phenomenology · Physics 2023-04-12 Mads T. Frandsen , Martin Rosenlyst

Using the full set of the LHC Higgs data from the runs at 7 and 8 TeV center of mass energies that have been released by the ATLAS and CMS collaborations, we determine the couplings of the Higgs particle to fermions and gauge bosons as well…

High Energy Physics - Phenomenology · Physics 2015-06-15 Abdelhak Djouadi , Grégory Moreau

We estimate the top quark, lightest sparticle (LSP) and scalar higgs masses within a supersymmetric grand unified framework in which $\tan\beta \simeq m_t/m_b$ and the electroweak symmetry is radiatively broken. The requirement that the…

High Energy Physics - Phenomenology · Physics 2011-05-12 B. Ananthanarayan , Q. Shafi

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

One year of Z- and WW-Threshold running of TESLA can provide the possibility to measure electroweak precision observables to an extremely high accuracy. At the Z peak O(10^9) Z bosons and about 6 10^8 b quarks can be collected. We employ…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Heinemeyer , Th. Mannel , G. Weiglein

Small momentum transfer elastic proton-proton cross-section at high energies is calculated assuming the nucleon composed of two constituents - a quark and a diquark. A comparison to data (described very well up to -t = 2 GeV^2/c) allows to…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Bialas , A. Bzdak

The relativistic quark model is presented. The quark-antiquark potential for the Schroedinger-like equation is constructed with the account of retardation effects and one-loop radiative corrections. It consists of the one-gluon exchange…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Ebert , R. N. Faustov , V. O. Galkin

We work out simple tree level relations in a top condensate model with dynamical electroweak symmetry breaking. We find that in this picture the mass of the composite Higgs boson at tree level is given by $m_H^2=\frac{m_t^2}{2}$ where $m_t$…

High Energy Physics - Phenomenology · Physics 2014-11-04 Amir H. Fariborz , Renata Jora , Joseph Schechter

The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. Dittmaier , M. Krämer , Y. Liao , M. Spira , P. M. Zerwas

Constraints on Wilson coefficients (WCs) corresponding to dimension-six operators of the standard model effective field theory (SMEFT) are determined from a simultaneous fit to seven sets of CMS measurements probing Higgs boson, electroweak…

High Energy Physics - Experiment · Physics 2026-04-06 CMS Collaboration

We re-examine our former predictions \cite{kahanath1,kahanath2} of the top and Higgs masses via dynamical symmetry breaking in a 4-fermion theory which produces the Higgs as a bound state, and relates the top and Higgs masses to $m_W$. The…

High Energy Physics - Phenomenology · Physics 2015-03-19 D. E. Kahana , S. H. Kahana

A search for a standard model Higgs boson produced in association with a top-quark pair and decaying to bottom quarks is presented. Events with hadronic jets and one or two oppositely charged leptons are selected from a data sample…

High Energy Physics - Experiment · Physics 2015-06-16 CMS Collaboration

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 composite Higgs boson of 125 GeV mass, only mildly fine-tuned, requires top partners with a semi-perturbative coupling and a mass not greater than about a TeV. We analyze the strong constraints on such picture arising from flavour and…

High Energy Physics - Phenomenology · Physics 2015-06-12 Riccardo Barbieri , Dario Buttazzo , Filippo Sala , David M. Straub , Andrea Tesi

Recent data indicate that $V_{ub}\cong \lambda^4 \cong (0.22)^4$, while $m_t$ seems to be $174$ GeV. The relations $m_d/m_s\sim m_s/m_b \sim \delta \sim \lambda^2 \simeq \vert V_{cb}\vert$ and $m_u/m_c\sim m_c/m_t \sim \delta^2 \sim…

High Energy Physics - Phenomenology · Physics 2010-11-01 Wei-Shu Hou , Gwo-Guang Wong