Part Three of the Interim In-Between Session 7 and 8 of Course 18

In so as to the divergent nature of an orbifold -- that is interially perturbated by the directly corresponding changes in the respective genus of the Hamiltonian-based nature -- of those superstrings that work to comprise the orbifold -- this format of kinematic inter-play works to produce a repulsion-based redistribution of the component eigenmembers of the directly inherent homotopic index, which tends to work to pull in the physical presence of group attractors.  This general type of activity tends to work to cause the here respective given arbitrary homotopic index -- of the topological condition of the so-stated orbifold, to bear a hightened tense of a fractal of magnetic-based qualities. This is since this genus of activity will work to increase the scalar magnitude of the Hodge-based index of the spin-orbital-based activities of the here directly corresponding superstrings -- that are here going through such an eluded-to change.  Whenever such a newly formed tense of superconformal invariance is altered relatively more rapidly, the potential for a hightened tense of change in the directly corresponding spin-orbital indices is bound to occur, at the here generally considered orbifold-based locus.  Yet, the less that various covariant superstrings act as being of a local tense, when this condition is to be of a bearing of one set of such superstrings relative to another set of such superstrings, the lower that the fractal of magnetism is -- that would then exist the one toward the other.  This latter tense of covariance, that acts as at more of a distance, will involve a weaker degree of homotopic interchange than if the tense of covariance were to instead  act at more of a local manner.  So, as an ansantz, magnetic flux density tends to be strongest when the eigenmembers that covariantly work to form such an inter-relation are local -- the one toward the other.  To be continued!  Sam Roach.