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

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''[https://youtu.be/Z7rd04KzLcg?t=7107 01:58:27]''<br>And that's not there, that was a mistake. Oh no, sorry. That was a mistake, calling it a mistake. These are two separate equations, right? So you have two separate fields, \(\nu\) and \(\zeta\), and you have a coupled set of differential equations that are playing the role of the Dirac theory, coming from the Hodge theory of a complex, whose obstruction to being [a] cohomology theory would be the replacement to the Einstein field equations, which would be rendered gauge invariant on a group relative to a tilted subgroup.
''[https://youtu.be/Z7rd04KzLcg?t=7107 01:58:27]''<br>And that's not there, that was a mistake. Oh no, sorry. That was a mistake, calling it a mistake. These are two separate equations, right? So you have two separate fields, \(\nu\) and \(\zeta\), and you have a coupled set of differential equations that are playing the role of the Dirac theory, coming from the Hodge theory of a complex, whose obstruction to being [a] cohomology theory would be the replacement to the Einstein field equations, which would be rendered gauge invariant on a group relative to a tilted subgroup.
[[File:Symm-Conn-Eq.jpg|center]]


''[https://youtu.be/Z7rd04KzLcg?t=7152 01:59:12]''<br>
''[https://youtu.be/Z7rd04KzLcg?t=7152 01:59:12]''<br>