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weak bosons

weak bosons. -. composite. H. Fritzsch LMU Munich. L H C. Z. ???. 126 GeV. Z. -. ??? „ Higgs “ boson. -. !!! excited weak boson spin 0. -. weak bosons composite. proton mass field energy ( gluons and quarks ). -. weak bosons. -. composite. -.

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weak bosons

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  1. weakbosons - composite H. Fritzsch LMU Munich

  2. L H C Z ??? 126 GeV Z

  3. - ??? „Higgs“ boson

  4. - !!! excited weakboson spin 0

  5. - weakbosons composite

  6. protonmassfieldenergy(gluonsandquarks)

  7. -

  8. weakbosons - composite

  9. - analogy

  10. 1954=> C.N. Yang, R. MillsJ. J. Sakurairhomesonselementarygaugebosons

  11. 1964massgenerationrhomesons„Higgs“mechanism

  12. - SU(2) 2 x 2 scalars mass M massless rho - mesons

  13. - “Higgs“ - mechanism „Higgs“ - scalar mass M massive rho - mesons

  14. rho – mesons 1964 Quark-antiquark …boundstates….

  15. - Q C D 1 GeV no „Higgs“ - scalar massive rho - mesons

  16. - no „Higgs“ - scalar massive weakbosons

  17. - lefthandedfermions

  18. haplos simple

  19. - electric charges

  20. -

  21. - haplons confined by gauge force QHD chiralgaugetheory

  22. - gaugegroup ofQHD SU(2)

  23. - massscale of QHD

  24. - Mixing W-boson - photon

  25. mixingparameter

  26. - ~10.4 GeV

  27. - QHD

  28. - QHD + QED ~10.4 GeV

  29. Standard Theory

  30. - W decay constant

  31. -

  32. - -

  33. c o m p l e x i t i e s of strong interactions ~ 1 G e V

  34. complexities of Q H D interactions ~ 1 TeV

  35. Excitedweakbosons

  36. p-wavebosons three SU(2) singlets S(0) = 0 (0) S(1) = 0 (1) S(2) = 0 (2)

  37. p-wavebosons three SU(2) triplets T(0) = 1 (0) T(1) = 1 (1) T(2) = 1 (2)

  38. p-wavemesons( QCD )isospinsinglets

  39. isospintriplets in QCD

  40. 1 GeV 0.5 GeV

  41. analogy

  42. 0.5 TeV ? 0.1 TeV

  43. - S(0) LHC 126 GeV

  44. S(0) 126 GeV

  45. 0.5 TeV 0.1 TeV

  46. 0.5 TeV 0.1 TeV

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