Noether-Based Reverberation

How about if we chose the initial conditions of one respsective given arbitrary orbifold eigenset, to be of an accelerating nature -- as it is gradually increasing in its Noether Current, which is as the directly corresponding tense of its correlative Majorana-Weyl-Covariance is to here, as well, be going through a Ward-Caucy-based tense of a correlative gradual state of a gradual loosening of the directly corresponding cohomological inhibition of the said orbifold eigenset.   This orbifold eigenset is to act as if it is of the conformally invariant condition of the integrative Hodge-based Fourier-related behavior, that is of those eigenindices that are to work here as the resultant metrical-gauge-based Hamiltonian operation, that is of the Gliosis-based interdependent group-field of the correlative sum of the discrete quanta of energy that has then come together -- in so as to work to form the directly associated group of superstrings of such a given arbitrary respective case scenario. This happens in so as to operate, to help form one overall group-related function.  Let us next consider, that, after a relatively transient set of a sequential series of group-related instantons, that the so-stated orbifold eigenset of this case, is to make a Gliosis-based contact with an external field -- to where the said eigenset is to then act in such a manner, in so as to reverberate back into the opposite direction that it was initially traveling through.  Let us say, that upon the immediate Yukawa-based contact of the so-stated orbifold eigenset with the said external field, that this so-stated field will then work here as a barrier -- that is phenotypically to remain relatively stationary upon contact, to where it may be deemed that both the directoral-based topological sway, and also the directoral-based sum of both the angular momentum and the spin-orbital momentum of each of the individually taken discrete quanta of energy -- that work here, in so as to help to form the behavior of that tense of the respective given arbitrary Majorana-Weyl-Covariant-Mode, to where the correlative orbifold eigenset is to reverse in direction, via the reformation of its operational indices --to where those respective functional operations, that had worked to initially helped to form the Ward-Caucy conditions that had initially worked to form the initial so-stated Noether Current, is to then be reversed in its course of action, yet, with both an identical reverse-holomorphic topological wave-tug/wave-push, as well as being drawn into the same course of the gradual loosening of the respective tenses of its correlative Majorana-Weyl-Covariance.  This will then work to form a gradual increase in the directly associated Noether Current, -- yet both from the opposite end of the directly affiliated and so-eluded-to semi-infinite Real Reimmanian quantum well, as "well" as then working to help to cause the then accelerating orbifold eigenset, to then go from the initial rate that the said eigenset had been initially extrapolated at as, although in this case when going from the relatively opposite end of the quantum well, towards the relatively initial end of the said quantum well.  After the said orbifold eigenset is to susequently strike the initially so-eluded-to end of the quantum well -- which was that extrapolated end to where such a case was to have its initial instant under consideration at -- to where this whole process is to then reiterate.  One may then call such an iterative process -- a Noether-based reverberation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.