Part Two As To Certain Substringular Perturbations

Those interactions that appertain to the convergence of certain substringular phenomenology that act as proximal indices of covariant Hamiltonian operators, that function as one whole matrix or manifold of substringular holonomic substrate, in such a manner in so as to perform one given arbitrary respective specific function as an orbifold eigenset -- act as metrical-based eigenstates that are directly correlative to the same group attractor eigenmetric, over the corroberative sequential series of group-related instantons.  This codeteminable and codifferentiable tendency of kinematic interdependence works to make the so-stated substringular phenomenology discussed here to be of one common eigenbase of orbifold eigenset, in what will here work to cause the so-eluded-to inherent substringular tense of holonomic substrate to act as a closely-knit genus of interactive operation -- and of which also causes the Hodge-Index of the directly corresponding fractal of magnetic-based pull to be of a relatively large discrete quantum -- in the form of a relatively dense Hodge-based spin-orbital kinematic operational scalar magnitude.  After many iterations and reiterations of the correlative superstrings, that are here within their conformally invariant loci of substringular neighborhoods -- these neighborhoods of which are of their localized sequences, works to cause the just-eluded-to fractal of magnetism that is of their convergent wave iteration to emit residual flux -- in the form of what may termed of as transpositional waves that may be extrapolated by a genus of a Sterling Approximation.  These so-stated transpositional waves interact with the kernels that would exist in the here respective corresponding Hamiltonian-based operands -- these being the kernels as to the fractal of the magnetic flux density of the so-stated given arbitrary superstrings of discrete energy permittivity, that I have described in this said case scenario.  As the so-eluded initially Majorana-Weyl-Invariant conformal-based region -- in which the so-stated one million respective given arbitrary superstringular Hamiltonian operators have been delineated and redelineated over the so-eluded-to group-metric in which these said superstrings have acted as a conformally invariant orbifold eigenset, begin to diverge -- the consequent polymorphism of the strings surrounding the so-eluded-to group attractor eigenmatrix will then here relatively diverge from the coniaxial interplay, as to where the generation of the directly corresponding wave-tug/wave-pull has its maximum scalar amplitude.  As such a divergence happens to the Hamiltonian operators that had worked to form the so-stated orbifold eigenset, the eigenbasis that works to describe the manner as to the sequential reiteration that had directly appertained to the prior mentioned superstrings of discrete energy permittivity -- alters or perturbates from both the earlier morphological genus, as well as the earlier kinematic-based genus -- that such directly correlative superstrings had demonstrated before.  I will continue with the suspense later! Sam.