Entropy And Cohomological Degeneration

Let us initially consider a photon of a beam of light, that is to strike an electron, that is of a set of atoms that are here to work to comprise a gauged overall mass-bearing phenomenology.  As the said photon is to strike the externalized core-field-density of a light-cone-gauge eigenstate of the electron that the so-stated photon is to collide with, in what is here to be in a Gliosis-based manner, -- that particular light-cone-gauge eigenstate of that discrete quantum of energy of the correlative electron that the said photon is to strike, -- is to initially -- upon its Gliosis-based collision with the said externalized core-field-density of the said light-cone-gauge eigenstate -- to become of an entropic-based manner, for an overall course of 384 consecutive iterations of group-related instantons, --in so long as the so-stated photon is not to collide with the externalized core-field-density of the holonomic substrate of any other light-cone-gauge eigenstate.  As the so-stated photon is to behave in an entropic-based manner, the said entropic photon is to tend to purely degenerate the cohomological stratum that it is to interact with, in a Yukawa-based manner.  Entropy never tends to bear the tense of being conformally invariant -- at the internal reference frame at which it is here to be operational chaotic or entropic in its behavior here.  An entropic condition is a condition of chaos or disorder.  Disorder or chaos is not of an organized manner, when the processes of such chaos is entropic or out of order or out of organization.  Disorder or chaos works to disorganize things.  Disorganization thus works to degenerate cohomological stratum, at the Ward-Cauchy level that is Poincare to the processes of its said disorganization.  Therefore, entropic photons are examples of photons that are here to be perturbated into a Rayleigh-based state of a scattering mode.  Entropic photons that are adjacent, will thus tend to bear an odd chirality-based parity -- over any correlative gauged group-metric that is of an even Hamiltonian operation.  Thus, the re-quantization of photons that were once entropic -- to where the said re-quantized photons are to then to return to a tense of working to bear a harmonic order -- is an example of a Reimman scattering, that is to bear photons that are no longer entropic in a discrete arrangement, in which the adjacent correlative eigenindices of the discrete electromagnetic quantum of energy are here to bear an even chirality-based parity.  (Now that such a discrete quantum of electromagnetic energy is to no longer be entropic.)  I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.