SU(5) - Institute of Particle and Nuclear Physics

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Building the Fermion Multiplets IISM multiplets:⎛⎝u cu cu c16⎞d cd c ⎠d c⎛ ⎞u⎝u⎠u⎛ ⎞d⎝d⎠d(ecν c )23− 1 3− 1 2−1e
Building the Fermion Multiplets IISM multiplets:⎛⎝u cu cu c⎞d cd c ⎠d c⎛ ⎞u⎝u⎠u⎛ ⎞d⎝d⎠d(ecν c )e16⎛ ⎞dd<strong>SU</strong>(5) multiplets: 5:⎜ d⎟⎝e c ⎠ν c23− 1 3− 1 2−1
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 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 48 and 49: ResultsMinimalisation Conditions:
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

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