Difference between revisions of "A Portal Special Presentation- Geometric Unity: A First Look"
A Portal Special Presentation- Geometric Unity: A First Look (view source)
Revision as of 01:15, 12 April 2020
, 01:15, 12 April 2020→Part II-B: Unified Field Content Plus a Toolkit
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<p>[01:40:08] Well, because the curvature. | <p>[01:40:08] Well, because the curvature. | ||
<p>[01:40:22] So you have Shiab | <p>[01:40:22] So you have Shiab because the curvature of a connection hit by a gauge transformation is equal on the nose. | ||
<p>[01:40:42] adjoint action on the lie algebra of the curvature. We know that if we have two possible actions of conjugation under a bracket and the bracket respects the action of the gauge group, we know that this is going to be well preserved. In other words, we're going to get a form that is gauged in variant relative to the tilted gauge group. | |||
<p>[01:40:42] adjoint action on the lie algebra of the curvature. We know that if we have two possible actions of conjugation under a bracket and the bracket | |||
<p>[01:41:08] And so as a result, we now have the possibility for equations of motion, which are well-defined. Uh, even though they involve projection operators, because we've built the symmetries into the theory and we're working on a group manifold to begin with. | <p>[01:41:08] And so as a result, we now have the possibility for equations of motion, which are well-defined. Uh, even though they involve projection operators, because we've built the symmetries into the theory and we're working on a group manifold to begin with. | ||