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SUMMARY:Jarek Duda (JU)
DTSTART:20240601T140000Z
DTEND:20240601T160000Z
DTSTAMP:20260423T011055Z
UID:QMFNoT/54
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/QMFNoT/54/">
 Geometric interpretation of the Standard Model as topological excitations<
 /a>\nby Jarek Duda (JU) as part of QM Foundations & Nature of Time seminar
 \n\n\nAbstract\nIn perturbative QFT we decompose scenarios into Feynman en
 semble of diagrams\, each of them should correspond to a field configurati
 on - I would like to present and discuss geometric/topological approach to
  find them\, based on liquid crystal Landau-de Gennes model. To enforce ch
 arge quantization in Gauss law\, we interpret dual F tensor as curvature o
 f a deeper field (Faber’s approach)\, this way Gauss law counts its topo
 logical charge. To prevent infinite energy of singularity in its center\, 
 we use Higgs-like potential to regularize it to a finite energy (mass)\, w
 hat leads to short range corrections of Coulomb interaction\, in agreement
  with the running coupling effect (arXiv:2210.13374). Living in 3D\, charg
 es appear in 3 families of different mass\, resembling 3 leptons. There ar
 e also 3 types of vortices resembling color strings - which inward/outward
  field rotation by pi would correspond to elementary electric (as topologi
 cal) charge\, and fractional rotations to 6 types of quarks\, e.g. appeari
 ng in quark-antiquark pairs with increased energy between them for confine
 ment. The u quark is preferred energetically due to suggested baryon confi
 guration\, explaining why proton is lighter than neutron\, also e.g. bindi
 ng mechanism and electric quadrupole moment of deuteron. Hadronization can
  be viewed here through reconnections of such high energy color string int
 o various final configurations. Suggested neutrino oscillations through fi
 eld rotations also seem in agreement: mainly between muon and tau neutrino
 \, with more freedom in PMNS than CKM mixing matrices.\n
LOCATION:https://researchseminars.org/talk/QMFNoT/54/
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