Difference between revisions of "A Portal Special Presentation- Geometric Unity: A First Look"
A Portal Special Presentation- Geometric Unity: A First Look (view source)
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<p>[01:41:58] So, neither this term nor this term is invariant. But they fail to be gauge invariant in exactly the same way. So, an important principle of life, which I took too long to realize is that if you have one disease, you're in real trouble. But if you have two diseases, you always have the possibility of having one disease kill the other disease. | <p>[01:41:58] So, neither this term nor this term is invariant. But they fail to be gauge invariant in exactly the same way. So, an important principle of life, which I took too long to realize is that if you have one disease, you're in real trouble. But if you have two diseases, you always have the possibility of having one disease kill the other disease. | ||
<p>[01:42:16] This is true in [Renormalization theory]. It's true in [Black-Scholes] theory. It's true all over the place. So, what we have here is we've gotten more diseases into the theory, but an even number of diseases allow us to have no disease at all. So, now we have two great tensors. We've got one tensor coming from the curvature and Shiab operator. | <p>[01:42:16] This is true in [[Renormalization theory]]. It's true in [[Black-Scholes]] theory. It's true all over the place. So, what we have here is we've gotten more diseases into the theory, but an even number of diseases allow us to have no disease at all. So, now we have two great tensors. We've got one tensor coming from the curvature and Shiab operator. | ||
<p>[01:42:34] We have another tensor coming from the torsion and its augmentation. | <p>[01:42:34] We have another tensor coming from the torsion and its augmentation. |