A Portal Special Presentation- Geometric Unity: A First Look: Difference between revisions
A Portal Special Presentation- Geometric Unity: A First Look (edit)
Revision as of 23:15, 11 April 2020
, 11 April 2020→Part III: Starting in on Physics
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<p>[01:47:14] With a copy of the one forms tendered in the spinors, and let me come up with two other copies of the same data. | <p>[01:47:14] With a copy of the one forms tendered in the spinors, and let me come up with two other copies of the same data. | ||
<p>[01:47:32] So I'll make Omega D minus one just by duality. So imagine that there's a [ | <p>[01:47:32] So I'll make Omega D minus one just by duality. So imagine that there's a [[Hodge star]] operator. | ||
<p>[01:47:43] And , whereas a little kid, I had the [https://en.wikipedia.org/wiki/Soma_cube Soma cube]. I don't know if you've ever played with one of these things. They're fantastic. And, uh, I later found out that this guy who invented the Soma cube, which you had to put together as pieces, there was one piece that looked like this, this object. And he was like this amazing guy | <p>[01:47:43] And , whereas a little kid, I had the [https://en.wikipedia.org/wiki/Soma_cube Soma cube]. I don't know if you've ever played with one of these things. They're fantastic. And, uh, I later found out that this guy who invented the Soma cube, which you had to put together as pieces, there was one piece that looked like this, this object. And he was like this amazing guy in the Resistance during World War II. | ||
<p>[01:48:03] So I would like to name this, the Somatic Complex. after, I guess his name is I think | <p>[01:48:03] So I would like to name this, the Somatic Complex. after, I guess his name is Piet Hein, I think. So this complex, I'm going to choose to start filling in some operators, the exterior derivative coupled to a connection, but on the case of spinors, we're going to put a slash through it. Let's make this the identity. | ||
<p>[01:48:26] We'd now like to come up with a second operator here. Here in this second operator here should have the property that the complex should be exact and the obstruction to it being a true complex to nillpotency should be exactly the generalization of the Einstein equations. Thus unifying the spinnorial matter with the intrinsic replacement for the curvature equations. | <p>[01:48:26] We'd now like to come up with a second operator here. Here in this second operator here should have the property that the complex should be exact and the obstruction to it being a true complex to nillpotency should be exactly the generalization of the Einstein equations. Thus unifying the spinnorial matter with the intrinsic replacement for the curvature equations. | ||