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''[https://youtu.be/Z7rd04KzLcg?t=4435 01:13:55]''<br> | ''[https://youtu.be/Z7rd04KzLcg?t=4435 01:13:55]''<br> | ||
But now, as \(\theta\) changes, the fermions are defined on the chimeric bundle, and it's the isomorphism from the chimeric bundle to the tangent bundle of the space \(U\), which is variant—which means that the fermions no longer depend on the metric. They no longer depend on the \(\theta\) connection. They are there if things go quantum mechanical, and we've achieved our objective of putting the matter fields and the spin- | But now, as \(\theta\) changes, the fermions are defined on the chimeric bundle, and it's the isomorphism from the chimeric bundle to the tangent bundle of the space \(U\), which is variant—which means that the fermions no longer depend on the metric. They no longer depend on the \(\theta\) connection. They are there if things go quantum mechanical, and we've achieved our objective of putting the matter fields and the spin-1 fields on something of the same footing. | ||
====== Observerse Conclusion ====== | ====== Observerse Conclusion ====== |