When a photon is to strike a mass-bearing discrete quantum of energy -- the said photon is then to tend to strike the externalized core-field-density that is of the light-cone-gauge eigenstate that is of that self-said mass-bearing discrete quantum of energy. Two immediately adjacent superstrings that are of the same universal setting will tend to be orthogonal to one another, in a Ward-Cauchy-related manner. So, when a photon is to strike a mass-bearing discrete quantum of energy in a viable manner, that is as well of a Gliosis-related manner -- the collision of the said photon with the mass-bearing quantum, is to be of an orthogonal manner, and in the so-eluded-to Ward-Cauchy-based manner over time. As the said photon is in the process of colliding with the said discrete quantum of mass-bearing energy, the said externalized core-field-density that is of the light-cone-gauge eigenstate that is being struck here (the light-cone-gauge eigenstate of a discrete quantum of energy is the relatively wave-based phenomenology of the discrete energy impedance of the said given arbitrary discrete quantum of energy), -- this so-eluded-to impartation of force that is thus convened, will work to alter the "plucking" activity of the correlative gauge-bosons upon the correlative second-order light-cone-gauge eigenstates -- that are here of the directly corresponding mass-bearing discrete quantum of energy. This will then often work to alter the scalar amplitude of the resultant implementation of the correlative formation of Schwinger-Indices that are thence formed by the said discrete quantum of mass-bearing energy over time. As this is happening, the correlative electron -- of which is comprised of the orbifold eigenset that had here to have just contained that superstringular phenomenology that had just been struck -- will drop back-and-forth an energy level, in so as to work to release its residual discrete kinetic energy in the form of a discrete quantum of electromagnetic energy. When there are a large number of such collisions of photons upon a proximal localized set of mass-bearing quanta of discrete energy -- over a discrete evenly gauged Hamiltonian eigenmetric, those discrete quanta of electromagnetic energy that will tend to be produced, will usually tend to be primarily those photons that are here to be of an infrared or heat-based nature. Thus, the application of light upon a mass may often work to both increase the heat of the mass, as well as working to effect the proximal local condition of the Ricci Scalar eigenstates that are here to be locally attributed to such a given arbitrary case.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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