5,849
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We're doing okay. | We're doing okay. | ||
==== Swervature and Swerve with Shiab Operators ==== | ===== Swervature and Swerve with Shiab Operators ===== | ||
''[https://youtu.be/Z7rd04KzLcg?t=6186 01:43:06]''<br> | ''[https://youtu.be/Z7rd04KzLcg?t=6186 01:43:06]''<br> | ||
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So that's pretty cool. If that works, we've now taken the Einstein equation and we've put it not on the space of metrics, but we've put a generalization and an analog on the space of gauge potentials, much more amenable to quantization, with much more algebraic structure and symmetry in the form of the inhomogeneous gauge group and its homogeneous vector bundle, some of which may be supersymmetric. | So that's pretty cool. If that works, we've now taken the Einstein equation and we've put it not on the space of metrics, but we've put a generalization and an analog on the space of gauge potentials, much more amenable to quantization, with much more algebraic structure and symmetry in the form of the inhomogeneous gauge group and its homogeneous vector bundle, some of which may be supersymmetric. | ||
==== Somatic Complex and Two More Operators ==== | ===== Somatic Complex and Two More Operators ===== | ||
[01:46:44] Now, the question is: "We've integrated so tightly with the matter field" -- we have to ask ourselves the question -- "can we see unification here?" | [01:46:44] Now, the question is: "We've integrated so tightly with the matter field" -- we have to ask ourselves the question -- "can we see unification here?" |