Difference between revisions of "A Portal Special Presentation- Geometric Unity: A First Look"

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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: $$\Epsilon$$ 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>[01:36:04] 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.
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