Wednesday, October 12, 2016

A Further Interim As To Session 2 Of Course 20 -- Calabi Manifolds Calabi Interactions

If the Ward-Caucy-based Yukawa Coupling, that is of one set of zero-norm-state-projections, that are to strike one superstring of discrete kinetic energy permittivity, in so as to work to form a photon via the Fujikawa Coupling -- is to strike the just mentioned superstring at one given arbitrary angle, as would here be subtended from in-between the correlative said set of zero-norm-state-projections and the correlative Fadeev-Popov-Trace eigenstate -- the directly corresponding angle, that is to here be delineated by the directly corresponding individually taken set of zero-norm-state-projections, that are to here strike the correlative counterstring of discrete kinetic energy permittivity, by which this is to result in forming the directly corresponding counterpart of the said photon, via the Fujikawa Coupling -- this will happen, to where this is to then be subtended by the same genus of a Ward-Caucy-based angle, from in-between the correlative said set of zero-norm-state-projections and the correlative core-field-density of the directly corresponding superstring, that was here initially mentioned as working to form the so-stated photon.  If the so-eluded-to angle of Gliosis-based strike, is to be either more acute or more obtuse than it should theoretically be, in so as to work to form the initially extrapolated tense of the holomorphic pulse -- that the soon forming photon and its counterpart were to have -- in order to not veer in its directoral-based propagation, then, the holomorphic direction of the soon propagated photon and its counterpart will contorsion, as I will soon explain later!
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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