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''[https://youtu.be/Z7rd04KzLcg?t=6086 01:41:26]''<br> | ''[https://youtu.be/Z7rd04KzLcg?t=6086 01:41:26]''<br> | ||
What about the torsion? Can we rescue the torsion? Here, again, we have good news. The torsion is problematic, but if I look at a different field—which I'm going to call the '''augmented torsion''', and I define it to be the regular torsion, which would be \(\ | What about the torsion? Can we rescue the torsion? Here, again, we have good news. The torsion is problematic, but if I look at a different field—which I'm going to call the '''augmented torsion''', and I define it to be the regular torsion, which would be \(\Pi\) minus this expression, this turns out to be beautifully invariant again. | ||
<div style="text-align: center; margin-left: auto; margin-right: auto;">$$ T_{\epsilon, \pi} = \ | <div style="text-align: center; margin-left: auto; margin-right: auto;">$$ T_{\epsilon, \pi} = \Pi - h^{-1}d_{A_0}h $$</div> | ||