Part Two as to The Fractal of Magnetic Field

When there is an application of a relatively small quantum of reverse magnetism that is pulled into any given arbitrary substringular-based region in which there are superstrings of discrete energy permittivity -- that are Gliossi to the here directly corresponding Hamiltonian operands, the arrangement of those wave-based propagations hat are pulled into one sort or another of either a euclidean and/or a Clifford-based Expansion of the directly associated fractals of magnetism, in the form of core-field-density that is pulled and/or tugged around by the here so-eluded-to surrounding core-field-density of the surrounding substringular phenomena of the general region, in which such so-stated reverse magnetism is being delineated at, over the directly affiliated group associated metric -- that are subtended from the just mentioned and eluded-to superstrings and their counterstrings -- the initial genus of arrangement of the wave-functionability of discrete energy permittivity that had here initially corresponded to the arrangement of the pointal-based-functionabiligy of the correlative discrete energy permittivity, will tend to alter or perturbate in the general format of its so-eluded-to genus, over that ensuing sequential series of group-based instantons in which such an application of reverse-based magnetism is pulled into the here so-stated substringular neighborhood in which the so-stated superstrings and their corresponding counterstrings had been initially iterating at per instanton -- given the degree and/or manner of both the correlative covariant-based mode, its correlative codetermination, and, its correlative codifferentiation, over that time frame in which such a respective given arbitrary application is brought into the Ward-Caucy bounds of the Poincaire-based field that is Gliossi to the said core-field-density of the initially so-stated superstringular scenario.  Yet, if the region of interaction of such a case, as a whole, is not, in general, covariantly expanded into a divergent propagation of indical singularities that are then obviously not initially piecewise continuous, such a genus of a Rayleigh-based scattering of subtended wave-based delineations will here tend to not bring about annhilation-based tensors into the here so-eluded-to Gliossi-based field structure of the resultant region of substringular neighborhood, due to the conditions that, what may be here viewed of as unpropagated variant geometric configurations will, at the relative exterior of the so-eluded-to perturbation of a fractal of magnetic-based eigenindices, tend to diverge in its multidirectoral-based Lagrangian-based expansion of eigenstates -- to where the so-eluded-to Majorana-Weyl-Invariant mode at the so-stated perimeter of such an interaction will then tend to be inculcated by the node/antinodal "sheathe", that will then surround the relatively furthest extension of such an interaction, thereby bringing in an ensuing relatively local condition of a potentially piecewise continuous mode of  interactive eigenindices  -- slowing the resultant perturbated mode of such an eluded-to multiplicit Hamiltonian operator-like eigenstate -- that is of an altered spin-orbital-based Hamiltonian operation of superstrings, into a settled tense of covariant-based superstrings, that will then here tend to reattain more of a general tense of conformal invariance.
I will continue with course 18 next!  Sincerely, Sam.  To Be Continued!