Part One Of The Tenth Session Of Course Ten

Let's say that there were, in the following case scenario, three covariant substringular groups that are here going through a Fourier Transformation that is here perturbated in a Njenhuis manner in such a way to where the three said groups which here represent three orbifolds work to produce a alterior perturbation in the corresponding covariant differentiation that will potentially alter any potential Kaluza-Klein light-cone-gauge topology in the said three orbifolds to be brought into having a Yang-Mills light-cone-gauge topology.  Yet here, the homotopic residue of each mentioned substringular group will maintain its  Fourier-based generation of substringular field during the duration in which the said three mentioned groups propagate along the Ultimon Flow -- when one considers the integration of both the Real Reimmanian-based time that involves the reiterating of instantons along with the Imaginary-based time that exists in-between the durations of the said individual instantons over the course of the iteration and the reiteration of the integrated sequential series of instantons that form the time that involves the mentioned Fourier Transformaion illuded to here.  Homotopic residue is the mini-string segments that begin to break off while yet reconnect to other topology during what I term of as the space-hole.  The space-hole is the duration that happens right before the instanton-quaternionic-field-impulse-mode in which topology virtually disconnects in just of a manner in so that homotoy may be altered in just enough of a degree in order that norm-conditions may be able to change in the manner that these need to change so that the proper Gaussian Transformations may happen so that the substringular may be spontaneously and perpetually kinematic so that energy may be able to persist.  The prior activity that I was describing before I mentioned what homotopic residue is happens so thawt the previously mentioned homogeneous wave permittivity will allow for the commutation of spin symmetry via the indices that are relatively local to all three of the described substringular groups at one general group metric or another on their way through the Lagrangian-based operand that each group is kinematically pulled into through their motion along the Continuum.  Such an activity allows for the said three substringular groups to here differentiate in a timewise manner with what is in this case an even chirality that exists in an isometric fashion among the vibratory operation of the homotopic residue that respectively exists in correspondence with the three said substringular groups when in covariant relation with each other.  This prior activity is happening in holonomic proportion, in terms of their corresponding Hodge-Indices and the parity of their respective fractal of angular momentum, in such a manner so that their related norm-conditions that are in transition are here to be in covariance with the fractal of angular momentum of each sector of the described homotopic residue.  In the meanwhile, the tri-local substringular encodements that help to determine the positioning of the corresponding superstrings along with helping to determine the positioning of said superstrings homotopic residue, here works to converge the coniaxial that is related to the conipoint that helps to define the relativistic center of the general activity that I am describing here so that the locus of the related orbifolds that represent the three substringular groups may be in isometric and Hodge proportion to the euclidean-based even distribution of their wave propagation and their respective residue over what may be described here as an inverse of a Clifford Expansion that brings the three orbifolds into an interactive-based region.  Those semi-groups that here arbitrarily commute a kinematic discharge of phenomena that is related to the superstrings that comprise the said orbifolds as the said orbifolds exist in relation to one another will here form spin-symmetries that become covaliant via wave coaxials that kinematically differentiate thru Lagrangians that occur over an arbitrary Fourier Transform.  I will continue with the suspence later!  Part Two Soon!  Sincerely, Sam.