SU(5) - Institute of Particle and Nuclear Physics

More documents

Recommendations

Info

ResultsMinimalisation Conditions:◮ 4 conditions◮ DTS and finetuning still present but protected by SUSY◮ α ∝ ɛ in agreement with SUSY not allowing tadpole contributions
ResultsMinimalisation Conditions:◮ 4 conditions◮ DTS and finetuning still present but protected by SUSY◮ α ∝ ɛ in agreement with SUSY not allowing tadpole contributionsHiggs Masses:◮ 15 Goldstone bosons (mass = 0)◮ 5 light Higgs bosons satisfying the MSSM tree-level relations◮ all other Higgses are very heavy (mass ∼ v)
Page 4 and 5: MotivationWhy GUTs?◮ SM is a very
Page 6 and 7: Embedding the Gauge GroupSM gauge g
Page 12: Embedding the Gauge GroupSM gauge g
Page 16 and 17: Building the Fermion Multiplets IFe
Page 18 and 19: Building the Fermion Multiplets IFe
Page 20 and 21: Building the Fermion Multiplets IIS
Page 22 and 23: Building the Fermion Multiplets IIS
Page 24 and 25: Breaking SU(5)Goal:Use well-known H
Page 26 and 27: Breaking SU(5)Goal:Use well-known H
Page 28 and 29: Potential for the HiggsesW = m 2 H
Page 34 and 35: Choosing the Vacuum Expectation Val
Page 36 and 37: Choosing the Vacuum Expectation Val
Page 38 and 39: Minimizing the Higgs PotentialProce
Page 40 and 41: Minimizing the Higgs PotentialProce
Page 42 and 43: Masses of HiggsesProcedure1. Evalua
Page 44 and 45: Remarks◮ minimal SU(5) gives SM l
Page 46 and 47: Adding SupersymmetryMotivation◮ e
Page 50 and 51: Summary◮ GUT theories provide a p
Page 52: Feynman Diagrams for Proton Decayno

SU(5) - Institute of Particle and Nuclear Physics

You also want an ePaper? Increase the reach of your titles

Delete template?

Save as template?