This is so that the previously mentioned homogeneous wave permittivity will allow for the commutation of spin symmetry via the indices that are local to all three substringualr groups at one group metric or another on their way thru the Continuum -- differentiating time-wise with the chirality of the residue as it vibrates thru, while being in proportion to the related norm-conditions that are in transition by being in covariance with the angular momentum of each sector of the mentioned substringular residue. In the meanwhile, the tri-local substringular encodements converge the locus of the related orbifolds in proportion to the euclidean-based even distribution of their wave propagation and residue.
I will do the third part of this discussion tommorrow! I will talk to you then. Sincerely, Sam Roach.
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