The Strong Nuclear Force as a Gauge Theory - Part 3: The Gluon Fields

The Strong Nuclear Force as a Gauge Theory - Part 3: The Gluon Fields

Richard Behiel via YouTube Direct link

0:00 Intro, Dirac Lagrangian Does not have Local SU3 Symmetry

1 of 11

1 of 11

0:00 Intro, Dirac Lagrangian Does not have Local SU3 Symmetry

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The Strong Nuclear Force as a Gauge Theory - Part 3: The Gluon Fields

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  1. 1 0:00 Intro, Dirac Lagrangian Does not have Local SU3 Symmetry
  2. 2 7:15 Modifying the Lagrangian with D_mu
  3. 3 19:22 Deriving the Transformation Rule for G_mu
  4. 4 32:42 Showing that the new Lagrangian has Local SU3 Symmetry
  5. 5 37:27 Exploring the Interaction Term, L_int
  6. 6 43:32 Why the Adjoint Transformation is a Thing
  7. 7 48:22 Proving that G_mu must be Hermitian
  8. 8 1:11:12 Shaving off the Traceful Part, so G_mu is in su3
  9. 9 1:19:27 The Gluon Fields
  10. 10 1:23:05 Our Model, so Far...
  11. 11 1:26:52 How to Bring G_mu to Life?

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