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DTSTAMP:20251213T132133Z
UID:FE855394-6AFD-4474-850C-2319921BA579
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DESCRIPTION:We revive the BCS idea of Weinberg and Salam on dynamical EW sy
 mmetry breaking and replace the Higgs sector of the EW gauge model of thre
 e fermion flavors (families) with the chiral gauge SU(3)f quantum flavor d
 ynamics (QFD) strongly coupled at a huge scale A. I. Anomaly freedom\ndema
 nds the BSM extension of the SM fermion sector by one EW-sterile neutrino 
 ve per flavor. Il. The QFD distinguishes flavors by arguably generating th
 ree different huge soft Majorana masses Mp~ A of vr\, and three different 
 very small soft Dirac masses my * A of SM fermions common to all four spec
 ies in each flavor. 1. Complete self-consistent spontaneous breakdown of S
 U(3)f XU(1) by three My implies : (i) All flavor gluons acquire masses ~ M
 f. (ii) There is the vR-composite pseudo-NG Majoron. (ili) There are three
  very heavy Ot vR-composite Higgs bosons. 2. Sponta- neous breakdown of th
 e EW symmetry SU(2)\, X U(1)y down to U(1)em by three mg\, in contrast wit
 h the Higgs mechanism\, implies: (i) There are three SM-fermion-composite 
 0* Higgs bosons\nhf. (ii) The W and Z gauge bosons acquire masses ~ g(Em?)
 / and ~ V(g+93)(=m})1/2 respectively i.e.\, there is no genuine Fermi scal
 e. III. The SM-fermion mass degeneracy in flavors is lifted in terms of th
 e weak hyper-charges and the ratios mf/mz\,w in the UV-finite dynamical EW
 \nperturbation theory of Pagels and Stokar.\n\nJiří Hošek\n\nIEAP\, CTU
  in Prague\, Husova 240/5\, Prague\, Czech Republic\, Czech Republic
LOCATION:IEAP\, CTU in Prague\, Husova 240/5\, Prague\, Czech Republic\, Cz
 ech Republic
ORGANIZER:andre.sopczak@cern.ch
SEQUENCE:4
SUMMARY:A BSM model of flavors
URL;VALUE=URI:https://events.vtools.ieee.org/m/522197
X-ALT-DESC:Description: <br /><p>We revive the BCS idea of Weinberg and Sal
 am on dynamical EW symmetry breaking and replace the Higgs sector of the E
 W gauge model of three fermion flavors (families) with the chiral gauge SU
 (3)f quantum flavor dynamics (QFD) strongly coupled at a huge scale A. I. 
 Anomaly freedom<br>demands the BSM extension of the SM fermion sector by o
 ne EW-sterile neutrino ve per flavor. Il. The QFD distinguishes flavors by
  arguably generating three different huge soft Majorana masses Mp~ A of vr
 \, and three different very small soft Dirac masses my * A of SM fermions 
 common to all four species in each flavor. 1. Complete self-consistent spo
 ntaneous breakdown of SU(3)f XU(1) by three My implies : (i) All flavor gl
 uons acquire masses ~ Mf. (ii) There is the vR-composite pseudo-NG Majoron
 . (ili) There are three very heavy Ot vR-composite Higgs bosons. 2. Sponta
 - neous breakdown of the EW symmetry SU(2)\, X U(1)y down to U(1)em by thr
 ee mg\, in contrast with the Higgs mechanism\, implies: (i) There are thre
 e SM-fermion-composite 0* Higgs bosons<br>hf. (ii) The W and Z gauge boson
 s acquire masses ~ g(Em?)/ and ~ V(g+93)(=m})1/2 respectively i.e.\, there
  is no genuine Fermi scale. III. The SM-fermion mass degeneracy in flavors
  is lifted in terms of the weak hyper-charges and the ratios mf/mz\,w in t
 he UV-finite dynamical EW<br>perturbation theory of Pagels and Stokar.</p>
 \n<p>Jiř&iacute\; Ho&scaron\;ek</p>
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