The Second of the Three Parts of the "Next" Session of Course Nine

The more that a Wilson Line develops in terms of having more of a basis of unitization among the superstrings that form the said two mentioned substringular groups taken individually -- and especially when such unitization combines the two said groups in a manner that potentially causes these to form a syncronization that wilil pull these into a motion that involves a discrete Lagrangain, the more that such a unitization may spontaneously allign the parity between these related superstrings of which would converge the arbitrarily related holonomic discharge of substringular field (mini-string fields) which, if the two Noether-Based flows of the two prior mentioned substringular groups catches up with the prior mentioned arbitrary tachyonic-based substringular group on account of what would appertain to a minor spuriousness in the tachyonic scattering of the substringular group that was Njenhuisly perturbated, then, the three groups which here represent three orbifolds will thus produce a perturbation in the related covariant codifferentiation that will potentially alter any potential Kaluza-Klein topology in the said three orbifolds into a Yang-Mills topology.  But, here, the homotopic residue of each mentioned substringular group will maintain its Fourier-based generation of substringular field as the said groups propagate along the Ultimon.  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 substringular groups at one group metric or another on their way thru the Continuum, differentiating timewise with the chirality of the residue as it vibrates. Such a wave permittivity will then be in proportion to the related norm-conditions that are in transition via a covariance with the angular momentum of each sector of the mentioned substringular residue.