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''[https://youtu.be/Z7rd04KzLcg?t=6421 01:47:01]''<br> | ''[https://youtu.be/Z7rd04KzLcg?t=6421 01:47:01]''<br> | ||
Let's define matter content in the form of Omega-0 tensored in the spinors, which is a fancy way of saying spinors, together with a copy of the one-forms tensored in the spinors. And let me come up with two other copies of the same data—so I'll make \(\Omega^{d-1}\) just by duality, so imagine that there's a Hodge star operator. | Let's define matter content in the form of Omega-0 tensored in the spinors, which is a fancy way of saying spinors, together with a copy of the one-forms tensored in the spinors. And let me come up with two other copies of the same data—so I'll make \(\Omega^{d-1}\) just by duality, so imagine that there's a Hodge star operator. | ||
[[File:InitialOmegaDiagram.jpg|center]] | |||
''[https://youtu.be/Z7rd04KzLcg?t=6463 01:47:43]''<br> | ''[https://youtu.be/Z7rd04KzLcg?t=6463 01:47:43]''<br> |