Friday, March 15, 2019

Some Cool Stuff About Reverberation Invariants

Reverberation Invariants -- what are these?  Here is one unique general genus, as to what a person may sometimes mean -- when they are here to refer to the term "reverberation invariants," -- when this is here to be taken at the substringular level.  Let us look at a closed string, that is here to be of a symplectic geometry, to where such a said superstring is here to be altering in its motion -- when this is in terms of its relationship, relative to light -- over the course of one given arbitrary set of iterations of group-related instanton.  After a certain brief evenly-gauged Hamiltonian eigenmetric, -- those partitions, that are here to work to involve the condition of that homotopic residue -- that is here to be directly related to the Polyakov Action that is pertinent to the relative motion of the said respective superstring of discrete energy permittivity, are then to tend to alter in their relative delineation and scalar amplitude -- as is according to the re-adjustment of the motion of the said superstring, when in relationship to both the motion and the existence of electromagnetic energy.  In the process, the proximal local Fock Space, that is of the given arbitrary respective region, will then tend to metaphorically act like a "spring" of seemingly disoriented first-order point particles, that are here to act, in so as to work to transfer a reverberation effect, that may here be thought of as a tense of a rippling effect, -- along the topology of the said string.  Entropy tends to be caused by the scattering of electromagnetic energy.  The Gliosis-related impact that is here to be formed,when electromagnetic energy is to scatter upon phenomenology -- tends to form an eminent effect upon the directly corresponding externalized core-field-density of those light-cone-gauge eigenstates, that will have thence to have just been struck by photon-related energy.  Such a direct impact, will thence tend to work to effect those vibrations that are to be formed by the plucking of second-order light-cone-gauge eigenstates by their correlative gauge-bosons.  This just mentioned tendency, will then tend to work to perturbate the nature of those Schwinger-Indices -- that are thence to be formed by the earlier so-stated plucking effect of gauge-bosons upon the said second-order light-cone-gauge eigenstates.  The quantization of Schwinger-Indices, that are propagated in such a manner -- that is both transversal and perpendicular -- as well as being of such a nature, in so as to then to work to bear a wavelength that is anywhere from between 5*10^(-22) of a meter to 4*10^(-18) of a meter in scalar magnitude, are what may be thought of as being the phenomenology of gravitational waves.  The activity of the relatively consistently occurring mingling of such gravitational waves, when this is here to be fractaled down to a level that may be more directly Yukawa to a superstring of discrete energy permittivity -- that is here to interact upon the topology of discrete energy in a ripple-like manner, over time, is what I had meant by the phrase, "reverberation invariants."
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

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