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Dynamical equations for fermion masses are derived using high scale universal mass generation and consequent mass evolution due to $SU(3), SU(2)$, and U(1$ gauge interaction. Assuming mass generation at the GUT scale $M=10^{14}$ GeV, one…

High Energy Physics - Phenomenology · Physics 2011-06-21 Yu. A. Simonov

We discuss a test of the Standard Model fermion mass origin in models of dynamical electroweak symmetry breaking. The couplings of composite pseudoscalar resonances to top quarks allow to distinguish high-scale Extended-Technicolor-type…

High Energy Physics - Phenomenology · Physics 2016-11-02 Tommi Alanne , Diogo Buarque Franzosi , Mads T. Frandsen

It is now established that the major source of electroweak symmetry breaking (EWSB) is due to the observed Higgs particle. However, whether the Higgs mechanism is responsible for the generation of all the fermion masses, in particular, the…

High Energy Physics - Phenomenology · Physics 2016-03-09 Diptimoy Ghosh , Rick Sandeepan Gupta , Gilad Perez

We propose a supersymmetric technicolor model in which the electroweak symmetry breaking is communicated to the quarks and leptons by technicolored $SU(2)_W$-singlet scalars. When the technifermions condense, the quarks and leptons of the…

High Energy Physics - Phenomenology · Physics 2008-12-22 Bogdan A. Dobrescu

We argue that in dynamical models of fermion masses, which explain the three mass scales of the generations of fermions with three separate heavy scales above the electroweak symmetry breaking scale, the off diagonal CKM matrix elements…

High Energy Physics - Phenomenology · Physics 2009-09-25 Nick Evans

In usual extended technicolor (ETC) theories based on the group ${\rm{SU}(N_{ETC}})_{ETC}$, the quarks of charge 2/3 and -1/3 and the charged leptons of all generations arise from ETC fermion multiplets transforming according to the…

High Energy Physics - Phenomenology · Physics 2011-02-01 Thomas A. Ryttov , Robert Shrock

We reconsider the question of mass generation for fermions coupled to a set of gauge bosons when the latter get their masses through the Goldstone bosons originating in a simple (i.e. not extended) technicolor sector. The fermion global…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. T. Tomboulis

In Topcolor theories the mass of the top quark is generated dynamically by new strong interactions coupling to the third generation fermions. This leads to potentially observable effects in flavor-changing neutral current processes…

High Energy Physics - Phenomenology · Physics 2007-05-23 Dimitris Kominis

The root of most of the technicolor (TC) problems lies in the way the ordinary fermions acquire their masses, where an ordinary fermion (f) couples to a technifermion (F) mediated by an Extended Technicolor (ETC) boson leading to fermion…

High Energy Physics - Phenomenology · Physics 2020-10-28 A. Doff

We consider a fully dynamical origin for the masses of weak gauge bosons and heavy quarks of the Standard Model. Electroweak symmetry breaking and the gauge boson masses arise from new strong dynamics, which leads to the appearance of a…

High Energy Physics - Phenomenology · Physics 2015-12-09 Stefano Di Chiara , Roshan Foadi , Kimmo Tuominen , Sara Tähtinen

We discuss fermion mass generation in unified models where QCD and technicolor (or any two strongly interacting theories) have their Schwinger-Dyson equations coupled. In this case the technicolor (TC) and QCD self-energies are modified in…

High Energy Physics - Phenomenology · Physics 2020-08-26 A. Doff , A. A. Natale

Precision measurements of the Higgs couplings are, for the first time, directly probing the mechanism of fermion mass generation. The purpose of this work is to determine to what extent these measurements can distinguish between the…

High Energy Physics - Phenomenology · Physics 2021-04-21 Michael J. Baker , Peter Cox , Raymond R. Volkas

A dynamical mechanism, based on a confining non-abelian dark symmetry, which generates Majorana masses for hypercharge-less fermions, is proposed. We apply it to the inverse seesaw scenario, which allows to generate light neutrino masses…

High Energy Physics - Phenomenology · Physics 2024-08-08 Maximilian Berbig , Juan Herrero-Garcia , Giacomo Landini

We describe a geometric picture for the pattern of fermion masses of the three generations which is invariant with respect to the renormalization group below the electroweak scale. Moreover, we predict the upper limit for the ratio between…

High Energy Physics - Phenomenology · Physics 2015-06-25 Salvatore Esposito , Pietro Santorelli

Despite the remarkable success of the Standard Model, the hierarchy and patterns of fermion masses and mixings remain a profound mystery. To address this, we propose a model employing the rank mechanism, where the originally massless quarks…

High Energy Physics - Phenomenology · Physics 2025-02-06 Sudip Jana , Sophie Klett , Manfred Lindner , Rabindra N. Mohapatra

A realistic technicolor model is presented with the dynamics below $150$ TeV treated explicitly. Electroweak symmetry is broken by the condensates of a `minimal' doublet of technifermions. The new feature of the model is that the the third…

High Energy Physics - Phenomenology · Physics 2009-09-15 Raman Sundrum

A spontaneously broken SU(2)xU(1) gauge theory with just one "primordial" generation of fermions is formulated in the context of generally covariant theory which contains two measures of integration in the action: the standard…

High Energy Physics - Theory · Physics 2014-11-18 E. I. Guendelman , A. B. Kaganovich

Assuming that the leptons and quarks other than top are massless at tree level, we show that their masses may be induced by loops involving the top quark. As a result, the generic features of the fermion mass spectrum arise from…

High Energy Physics - Phenomenology · Physics 2009-09-17 Bogdan A. Dobrescu , Patrick J. Fox

We investigate a local $SU(3)_F$ flavour symmetry for its viability in generating the masses for the quarks and charged leptons of the first two families through radiative corrections. Only the third-generation fermions get tree-level…

High Energy Physics - Phenomenology · Physics 2023-10-24 Gurucharan Mohanta , Ketan M. Patel

We suggest a mechanism explaining the origin of three generations of the Standard Model fermions from one generation in a higher-dimensional theory. Four-dimensional fermions appear as zero modes trapped in the core of a topological defect…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. V. Libanov , S. V. Troitsky
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