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 03:59, 11 April 2020
, 03:59, 11 April 2020→Part II: Unified Field Content
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<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 | <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, so we can define Dirac spinors on the chimeric bundle if we're in Euclidean signature. A 14-dimensional manifold has Dirac spinors of dimension-two to the dimension of the space divided by two. | ||
<p>[01:22:20] Right? So 2^14 over 2^7 is 128, so we have a map into a structured group of $$U^{128}$$ | <p>[01:22:20] Right? So 2^14 over 2^7 is 128, so we have a map into a structured group of $$U^{128}$$ | ||