The following simple model makes it possible to estimate the size of the effect of M4 Kähler force for elementary fermions at space-time level. Induced Dirac equation is assumed.
- Both nucleons and leptons create a classical induced M4 Kähler potential, which contributes to the U(1) part of the induced electroweak gauge potentials in the background space-time assignable to the nucleus.
- The gauge forces are felt at the light-like fermion lines at 3-D light-like partonic orbits. A string world sheet connecting say electron and nucleon could mediate the interaction.
- Consider 1-D light-like fermion line at the partonic orbit of a fermion. Idealize the fermion line as a light-like geodesic line in M4× S1, where S1⊂ CP2 is a geodesic circle. 8-D masslessness implies p2- R2ω2=0 (see this), where ω is expected to be the order of the particle mass and characterizes the rotation velocity associated with S1. A physically motivated guess is that ω is a geometric correlate for the Compton time of the fermion so that fermion can be said to have an internal clock.
- Consider M4 and CP2 contributions to the Kähler potential. Denote by u the CP2 coordinate serving as a coordinate for the fermion line at the partonic orbit as the interface between Euclidean CP2 type region identifiable as a wormhole contact connecting two Minkowskian space-time sheets and Minkowskian region. The CP2 part of the induced Kähler potential is of order ACP2u ∼ 1/R, where R is CP2 radius. The M4 part of the induced Kähler potential is AM4k∂ mk/∂u ∼ ω ∼ m. For electrons, the ratio of the two contributions is ω R ∼ me/m(CP2) ∼ 10-17 and therefore extremely small. This guarantees that the induced M4 Kähler form has negligible effects.
For a summary of earlier postings see Latest progress in TGD.
For the lists of articles (most of them published in journals founded by Huping Hu) and books about TGD see this.
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