Difference between revisions of "A Portal Special Presentation- Geometric Unity: A First Look"
A Portal Special Presentation- Geometric Unity: A First Look (view source)
Revision as of 23:14, 11 April 2020
, 23:14, 11 April 2020→Part II: Unified Field Content
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<p>[01:30:09] So just the way, when we look at supersymmetry, we can take products of the spin-one-half fields and map them into the linear sector. We can do the same thing here. So what we're talking about is something like a supersymmetric extension of the inhomogeneous gauge group analogous to supersymmetric extensions of the double cover of the inhomogeneous Lorentz or Poincaré group. Further, because this construction is at the level of groups, we've left a slot on the left hand side on which to act. So for example, if we want to take regular representations on the group, we can act by the group G on the left-hand side, because we're allowing the tilted gauge group to act on the right-hand side. | <p>[01:30:09] So just the way, when we look at supersymmetry, we can take products of the spin-one-half fields and map them into the linear sector. We can do the same thing here. So what we're talking about is something like a supersymmetric extension of the inhomogeneous gauge group analogous to supersymmetric extensions of the double cover of the inhomogeneous Lorentz or Poincaré group. Further, because this construction is at the level of groups, we've left a slot on the left hand side on which to act. So for example, if we want to take regular representations on the group, we can act by the group G on the left-hand side, because we're allowing the tilted gauge group to act on the right-hand side. | ||
<p>[01:30:56] So it's perfectly built for representation theory. And if you think back to Wigner’s classification and the concept that a particle should correspond to an irreducible representation of the inhomogeneous gauge group, uh, inhomogeneous Lorentz group, we may be able to play the same games here up to the issue of infinite dimentionality. | <p>[01:30:56] So it's perfectly built for representation theory. And if you think back to [[Wigner’s classification]] and the concept that a particle should correspond to an irreducible representation of the inhomogeneous gauge group, uh, inhomogeneous Lorentz group, we may be able to play the same games here up to the issue of infinite dimentionality. | ||
<p>[01:31:15] So right now, our field content is looking pretty good. It's looking unified in the sense. That it has an algebraic structure that is not usually enjoyed by field content and the field content from different sectors can interact and know about each other. Mmm. Provided we can drag something of this out of this with meaning. | <p>[01:31:15] So right now, our field content is looking pretty good. It's looking unified in the sense. That it has an algebraic structure that is not usually enjoyed by field content and the field content from different sectors can interact and know about each other. Mmm. Provided we can drag something of this out of this with meaning. | ||