On The Strong Force, In Terms Of The Weak Force

Let us say that there were to be a certain integer number of forces, that are to act upon an eigenstate of the strong force -- at a proximal localization, to the locus at which there is to be an eigenstate of the centralized knotting of the Rarita Structure, in the substringular.  Let us next say that there is to then be the introduction of a ghost-inhibitor -- to the general region at which the so-stated eigenstate of the  strong force was to be initially predominant at, in such a respective given arbitrary case scenario.  Let us next say, that such an introduction of the presence of the said ghost-inhibitor -- was to work to eliminate one or more of the so-eluded-to forces, by which the so-stated proximal locus of the said eigenstate of the strong force, that is of such a directly corresponding case, was to be differential at, in a Fourier-based manner, over an initially present sequential series of group-related instantons.  Let us then say, that the so-eluded-to physical removal of the said one or more forces -- that had worked, in so as to help to cause the here relatively proximal localized holonomic substrate of the said eigenstate of the strong force -- to then happen, to where this would then work in so as to cause an ensuing perturbation of the whole general locus of the said eigenstate.  This said eigenstate, that is of the centralized knotting of the relatively local eigenbase of the Rarita Structure, when this is taken in terms of the eigenbase of the initially so-eluded-to tense of that Majorana-Weyl-Invariant-Mode -- by which the said eigenstate of the strong force was to have here, had an initial consideration of working to bear a tense of superconformal invariance, from within the so-eluded-to initially considered Ward-Caucy bounds of the proximal localized mass-bearing state, by which the said eigenstate of the strong force was to here be working to help in the stability of what was to here be an eigenstate of a mass, that had initially been in a state of relative static equilibrium -- over a relatively transient duration of time. In such a given arbitrary case scenario, the so-stated elimination of the said one or more forces -- that had worked here, in so as to help in the process of the perpetuity of the so-eluded-to localized eigenstate of discrete mass -- may then often work to help at causing the initially bound condition of a relatively stable mass, that was here to be exhibiting the strong force, to then be locally unstable in its covariant eigenbase, as to its specific localization.  This may then happen, by which such a general condition -- will then be helping to work to cause the directly corresponding mass-bearing eigenstate, to then diverge from its initial state of superconformal invariance.  This may then often work to cause the resultant Ward-Caucy-based conditions of the directly corresponding eigenstate of mass -- that was  to initially be of a convergent nature,  when in terms of its initial state of conformal invariance -- to then work to tend to  bear a condition of spontaneous radioactive decay, thereby, to where this case scenario is to then, ironically enough, to move in the direction by which such a directly corresponding mass, is to then be exhibiting a given arbitrary case of the weak force, instead.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.