Part Three of the Seventh Session of Course 18

Any given arbitrary either conformally isolated superstring of discrete energy permittivity, or, any given arbitrary conformally isolated set of superstrings of discrete energy permittivity, that act in such a manner in so that these behave as kinematically acting in a codifferentiable way that is geometrically parallel in their relatively outer Ward-Neumman-based topological settings, with another of such a superstring or set of superstrings  -- can not, solely on their own account, propagate that fractal of their magnetism that is directly associated with the relatively intetial-based Hamiltonian operational-based spin-orbital indices, that these produce by their radial-based motions, over time.  Yet, if such a respective so-stated superstring or set of superstrings that are geometrically parallel with another of such a superstring or set of superstrings, at the Poincaire level of their exterial topological-based Ward-Neumman settings, works to bear one or more Njenhuis tensors -- that act in such a manner in so as to help the said dual condition of a superstring or set of superstrings to act in a covariant manner that is codeterminable, then, the directly corresponding Real Reimmanian directoral-based coniaxials will be facillitated to move more freely -- in so as to help to cause the norm-conditions of the correlative Majorana-Weyl-based substringular structures, that have been eluded-to here, to act as bearing a cubic Gaussian-based relationship, that will here kinematically inter-play as a multiplicit-based eigenstate in three or more spatial dimensions, over time.  So, when superstrings go from not spontaneously propagating their fractal of discrete magnetism -- to any viable extent -- to spontaneously propagating their fractal of discrete magnetism, to a viable extent -- in terms of the delineation of their Majorana-Weyl-related Hodge-based indices -- this is a tense of a cyclical-based Majorana-Weyl covaraince.  Since an orbifold works to involve a tense of a fractal of discrete magnetism, any given arbitrary orbifold, over time, alters in the manner of the production of its spin-orbital indices -- when in relationship to those spin-orbital indices that are produced by the surrounding orbifolds.  This is more of a general tense as to what a Majorana-Weyl covariant mode would happen to be.  When a conformally isolated string enters a manifold of other superstrings, this will work to involve a tense of a Majorana-Weyl covariance as well.   To Be Continued!  Sam Roach.