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

<p>[01:21:21] Furthermore, as we've said before, the ability to use projection operators together with the gauge group, is frustrated by virtue of the fact that these two things do not commute with each other. So now the question is, how are we going to prove that we're actually making a good trade?

<p>[01:21:21] Furthermore, as we've said before, the ability to use projection operators together with the gauge group, is frustrated by virtue of the fact that these two things do not commute with each other. So now the question is, how are we going to prove that we're actually making a good trade?

<p>[01:21:48] [The] first thing we need to do is we still have the right to choose intrinsic field content. [We] have an intrinsic field theory. So, if you consider the structure bundle of the spinors; we built the chimeric bundle, $$C$$, so we can define Dirac spinors on the chimeric bundle, if we're in Euclidean signature.

<p>[01:21:48] [The] first thing we need to do is we still have the right to choose intrinsic field content. [We] have an intrinsic field theory. So, if you consider the structure bundle of the spinors; we built the chimeric bundle, $$C$$, so we can define Dirac spinors on the chimeric bundle, if we're in Euclidean signature.