As an initially obvious statement -- electromagnetic energy not only scatters upon matter -- yet, it may also scatter upon plain kinetic energy as well. The process of electromagnetic energy scattering upon plain kinetic energy, may be thought of as being a Calabi-Wilson-Gordan interaction. Whenever light, or, whenever any electromagnetic energy if you will, is to be propagated through time and space, -- it is comprised of waves that are here to exist as a compilation of tiny discrete particles, that are known of as being called photons. An individual photon has, during any given arbitrary iteration of group-related instanton, located at a positioning that is coming from the said photons reverse-holomorphic side -- the existence of a Ward-Cauchy-related phenomenology, that may be described of here as being a Fadeev-Popov-Trace eigenstate. Such a said Fadeev-Popov-Trace eigenstate is here to be connected to the said discrete quantum of energy permittivity (the particle nature of the said "photons"), by manner of the so-eluded-to discrete quantum of energy -- by what may here be described of as a discrete first-order light-cone-gauge eigenstate. The superstring of such a photon is here to behave as being the discrete particle-based quantum of energy permittivity; the counter string of such a photon is here to behave as being the discrete wave-based quantum of energy permittivity; the Fadeev-Popov-Trace eigenstate of such a photon is here to behave as being the discrete particle-based quantum of energy impedance; And the first-order light-cone-gauge eigenstate of such a photon is here to behave as being the discrete wave-based quantum of energy impedance. When one is here to to in a Laplacian-based manner -- from the given arbitrary Fadeev-Popov-Trace eigenstate of a respective case to the counter string of the same respective given arbitrary counter string of such a said case, -- then, one is here to be going in a Laplacian-based manner, in the relative forward-holomorphic direction. With all of that in mind -- when a beam of electromagnetic energy is here to strike any given arbitrary field of plain kinetic energy, the so-eluded-to radiation may either become fully absorbed in the respective said entered field, or the radiation may be partially absorbed and partially scattered by the respective said entered field, or, the radiation may then become fully scattered by the respective said entered field. This will depend upon both the angle and the relative delineation of the said strike of the said radiation upon the said field of plain kinetic energy.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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