Let us say, that one is to have a substringular situation -- to where there is to be one Majorana-Weyl-Invariant-Spinor -- that is working to "try" to diverge from a second Majorana-Weyl-Invariant-Spinor, while the second mentioned spinor is to work to "try" to converge upon the first just mentioned spinor. Now -- let us say that there ensues to be a situation -- to where there is to be a third substringular entity, -- that acts upon the earlier mentioned scenario, to where the Fourier-related activities of the two different mentioned Majorana-Weyl-Invariant-Spinors are to coalesce into one group-acting Hamiltonian operator, after the particle that is here to act upon the two initially mentioned spinors, is to engage upon such an embarking in a Yukawa-related manner, over time. This would be one general genus of a group-attractor, which here may more specifically be named of as a gauge-attractor, as it is here to be a Ward-Cauchy-related substringular phenomenology -- that works at least in part, via the Fourier-related activity of potentially integrative Schwinger-Indices -- that are here to be propagated along the general Rarita Structure, over time. Again -- as an aside, such Schwinger-Indices (before these are here to coalesce into groups of such indices), are here to initially to be formed by the kinematic activity of gauge-bosons upon the topological stratum of the multiplicit light-cone-gauge.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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