Difference between revisions of "A Portal Special Presentation- Geometric Unity: A First Look"
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A Portal Special Presentation- Geometric Unity: A First Look (view source)
Revision as of 05:02, 11 April 2020
, 05:02, 11 April 2020→Part III: Unified Field Content Plus a Toolkit
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<p>[01:35:41] Now, this is a tremendous amount of freedom that we've just gained. Normally we keep losing freedom, but this is the first time we actually begin to see that we have a lot of freedom and we're going to actually retain some of this freedom to the end of the talk. But the idea being that I can now start to define operators which correspond to the "Ship in the Bottle" problem. | <p>[01:35:41] Now, this is a tremendous amount of freedom that we've just gained. Normally we keep losing freedom, but this is the first time we actually begin to see that we have a lot of freedom and we're going to actually retain some of this freedom to the end of the talk. But the idea being that I can now start to define operators which correspond to the "Ship in the Bottle" problem. | ||
<p>[01:36:04] I can take field content: $$\ | <p>[01:36:04] I can take field content: $$\epsilon$$ and $$\Pi$$, where these are elements of the inhomogeneous gauge group. In other words, where $$\epsilon$$, is a gauge transformation and $$\Pi$$ is a gauge potential. | ||
<p>[01:36:27] And I can start to define operators. | <p>[01:36:27] And I can start to define operators. | ||