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Related papers: Extended Technicolor Models with Two ETC Groups

200 papers

Against the conventional picture that the mass matrix forms in the quark sectors will take somewhat different structures from those in the lepton sectors, a possibility that all the mass matrices of quarks and leptons have the same form as…

High Energy Physics - Phenomenology · Physics 2017-08-23 Yoshio Koide , Hiroyuki Nishiura , Koichi Matsuda , Tatsuru Kikuchi , Takeshi Fukuyama

Starting from a characteristic biinvariance property of Higgs potentials in gauge theories with nonunitary parallel transporters, we explain how quarks of different flavor can acquire different masses by spontaneous symmetry breaking and…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. Lehmann , G. Mack , T. Prüstel

We consider the maximal U(3) horizontal scheme as a handle on fermion masses and mixings. In particular, we attempt to explain the large top Yukawa coupling and the masses and mixing in the two heaviest generations. A simple model is…

High Energy Physics - Phenomenology · Physics 2016-08-25 Andrija Rasin

We show that it is necessary to go beyond the BCS (rainbow-ladder) approximation to split the $\eta$ and $\eta'$ masses from the $\pi$ and K masses. We determine the self-consistent set of one-quark-loop diagrams both for the…

High Energy Physics - Phenomenology · Physics 2007-08-08 O. Lakhina , P. Bicudo

We review the connection between $m_t$ and the $Zb\bar b$ vertex in ETC models and demonstrate the power of the resulting experimental constraint on models with weak-singlet ETC bosons. Some efforts to bring ETC models into agreement with…

High Energy Physics - Phenomenology · Physics 2011-03-02 E. H. Simmons , R. S. Chivukula , J. Terning

We study the deep inelastic scattering and photo-production modes of $t\overline{t}$ pairs at the proposed LHeC and its potential to probe the electromagnetic and weak dipole moments (MDM and EDM for $tt\gamma$) of the top quark. A…

High Energy Physics - Phenomenology · Physics 2015-06-17 Antonio O. Bouzas , F. Larios

Models based on the extended $SU(3)_{C}\times SU(3)_{L}\times U(1)_{X}$ (331) gauge group usually follow a common pattern: two families of left-handed quarks are placed in anti-triplet representations of the $SU(3)_{L}$ group; the remaining…

High Energy Physics - Phenomenology · Physics 2016-08-11 Renato M. Fonseca , Martin Hirsch

Predictions for the angular distribution of massive quarks and leptons are presented, including QCD and QED corrections. Recent results for the fermionic part of the two-loop corrections to the electromagnetic form factors are combined with…

High Energy Physics - Phenomenology · Physics 2009-09-11 S. J. Brodsky , A. H. Hoang , J. H. Kuhn , T. Teubner

We consider a minimal technicolor model in which the ordinary and technicolor sectors are coupled by a {\it massless} scalar doublet. When technicolor interactions become strong, the resulting technicolor condensate not only breaks the…

High Energy Physics - Phenomenology · Physics 2009-09-11 Christopher D. Carone , Howard Georgi

The analysis of two-ordinary-meson scattering amplitudes in the limit of a large number $N_{\rm c}$ of the colour degrees of freedom of quantum chromodynamics, with suitably decreasing strong coupling and all quarks transforming according…

High Energy Physics - Phenomenology · Physics 2017-10-27 Wolfgang Lucha , Dmitri Melikhov , Hagop Sazdjian

We discuss the production of the exotic doubly-charmed tetraquark mesons ${\rm T}_{{\rm c}{\rm c}}({\rm c}{\rm c}\bar{\rm u}\bar{\rm d})$ from electron-positron collisions. ${\rm T}_{{\rm c}{\rm c}}({\rm c}{\rm c}\bar{\rm u}\bar{\rm d})$ is…

High Energy Physics - Phenomenology · Physics 2017-08-21 Tetsuo Hyodo , Yan-Rui Liu , Makoto Oka , Shigehiro Yasui

We propose a supersymmetric composite model with three generations in which supersymmetry and electroweak symmetry are broken dynamically, and masses of quarks and leptons are generated without introducing any mass scales by hand. All the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Noriaki Kitazawa

Topcolor-assisted technicolor provides a dynamical explanation for electroweak and flavor symmetry breaking and for the large mass of the top quark without unnatural fine tuning. I briefly review the basics of topcolor-assisted technicolor,…

High Energy Physics - Phenomenology · Physics 2007-05-23 Kenneth Lane

A colored weak singlet scalar state with hypercharge 4/3 is one of the possible candidates for the explanation of the unexpectedly large forward-backward asymmetry in $t \bar t$ production as measured by the CDF and D0 experiments. We…

High Energy Physics - Phenomenology · Physics 2011-11-03 Nejc Kosnik , Ilja Dorsner , Jure Drobnak , Svjetlana Fajfer , Jernej F. Kamenik

The scalar composite representations of the electroweak symmetry group of the Standard Model are exhibited in the case of two generations of quarks. The link between `strong' and `electroweak' eigenstates is investigated, showing that the…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Machet

We explore a scenarios where topcolor-like dynamics operates in the presence of fourth generation matter fields. Using the Minimal Walking Technicolor as a concrete basis for model building, we construct explicit models and confront them…

High Energy Physics - Phenomenology · Physics 2011-02-08 Hidenori S. Fukano , Kimmo Tuominen

If $c$ and $t$ quarks are strongly mixed with a weak singlet charge $2/3$ quark, $BR(t\to \ell\nu + X)$ could be suppressed via the $t\to cH^0$ mode, thereby the top quark could still hide below $M_W$, whereas the heavy quark signal…

High Energy Physics - Phenomenology · Physics 2009-10-28 Wei-Shu Hou , Hsuan-Cheng Huang

A vector-like extension of the standard model for heavier quarks and leptons with $SU(2)\times U(1)$ gauge symmetry and only one Higgs doublet is examined. This scheme incorporates infinitely many fermions and avoids the appearance of a…

High Energy Physics - Phenomenology · Physics 2017-02-01 Kazuo Fujikawa

We use the twist dimensions of the operators underlying the dynamical behavior of exclusive production processes as a tool for determining the structure of exotic heavy-quark states such as the $Z_c^+(4430)$ tetraquark. The resulting…

High Energy Physics - Phenomenology · Physics 2015-08-12 Stanley J. Brodsky , Richard F. Lebed

Ordinary technicolor and extended technicolor cannot produce the heavy top quark unaided. We demonstrate that a flavor-universal extension of the color interactions combined with an extended hypercharge sector that singles out the third…

High Energy Physics - Phenomenology · Physics 2016-08-25 Marko B. Popovic , Elizabeth H. Simmons
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