Light, or any other form of electromagnetic energy, can scatter upon either phenomenology of mass, phenomenology of plain kinetic energy, or upon phenomenology of other electromagnetic energy -- over time. When electromagnetic energy is to scatter upon another phenomenology, it is to strike the externalized core-field-density of the light-cone-gauge eigenstate of the discrete energy quantum -- that it is to come into contact with in the so-inferred Gliosis-based manner. Furthermore, any electromagnetic or electro-dynamic energy will tend to scatter upon any discrete quantum of mass, kinetic energy, and/or electromagnetic energy, in an initially Rayleigh-based manner -- when it is to strike the just inferred multiplicit externalized field of such a light-cone-gauge eigenstate, over any metric that may be gauged of as an even Hamiltonian operation, around the instance of contact, in which the so-eluded-to set of one or more photons are to make a direct Yukawa-based coupling upon the said phenomenology that may here be either as a quantum of a mass, a quantum of kinetic energy, and/or a quantum of electromagnetic energy, over time. This is particularly the case, when the phenomenology that is to be struck is in the Lagrangian-based path -- as to the mappable-tracing of the electromagnetic energy that is in its venue of moving in the direction of least time, as a Hamiltonian operand -- in which the photon or the photons that are to be scattered, are here to be "toggled" as is as according to Snell's Law. Mass-Bearing superstrings of discrete energy permittivity, that are in a state of superconformal invariance -- tend to be Yau-Exact. This is why I term those substringular manifolds, that are to be comprised of here as mass-bearing strings -- as Calabi-Yau manifolds. Electromagnetic superstrings of discrete energy permittivity, that are in a state of superconformal invariance -- tend to be partially Yau-Exact. This is why I term those substringular manifolds, that are to be comprised of here as electromagnetic strings -- as Calabi-Calabi manifolds. Furthermore, -- kinetic energy-bearing superstrings of discrete energy permittivity, that are in a state of superconformal invariance, tend to veer into a condition of bearing Chern-Simons singularities. This is why I call those substringular manifolds, that are to be comprised of plain kinetic energy -- as Calabi-Wilson-Gordan manifolds.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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