The Very Next Part of Session Five of Course 19 -- The Klein Bottle and Orbifold Differentiation

Let us now consider the Majorana-Weyl-Invariant-based field of the so-eluded-to given arbitrary orbifold, that I was beginning to describe earlier in this respective given session.  As the Majorana-Weyl-Invariant-based field that was so-mentioned, differentiates in a Fourier-based manner, as a mechanism that works to inter-relate a Hamiltonian-based operation -- that is of a spinning-twist-based torsion.   (The orbifolds that have here been brought into a conformally invariant-based setting -- bear a here relatively locally proximal, as well, set of spin-orbital Njenhuis tensors -- that operate in so as to kinematically differentiate off of here what is of the relative Real Reimmanian Plane, that is of the here directly corresponding Majorana-Weyl-Invariant-based field.  This happens, in so as to work to form a tense of a propagation, that is of the overall summed Hodge-Index -- that is of the Hamiltonian-based-operational fractals of the so-eluded-to magnetic field eigenbase of this respective given arbitrary case.  The here mentioned relatively proximal tense of indices -- that would here work to form the overall set of Hamiltonian operators, that would work in this case in so as to be what would here work to comprise the so-stated local fractal of magnetism, this of which is demonstrative in the set respective given arbitrary substringular neighborhood of this given case, acts, in so as to comprise that interconnection of the holonomic substrate of the said locally proximal orbifolds, that have here come together or integrated in so as to work to form the so-eluded-to regional orbifold eigenset of this respective given arbitrary case.  Theses said orbifolds, that have here come together in so as to form the given said orbifold eigenset -- are binded together via a tense of heterotic strings, that may be described of as E(8)XE(8) strings, these of which are of a heterotic nature, over time.  These said E(8)XE(8) heterotic strings, work to hold together the orbifolds of an orbifold eigenset, by proximally twisting as if these were gears, that operate in so as to bear a tensoric genus of substringular torque -- in such a manner that acts as is according to the scalar magnitude of the compactified slack of that wave-tug/wave-pull -- that acts here in an abelian manner, upon the holonomic substrate of the said heterotic E(8)XE(8) strings, these of which are, again an example of what are known of as heterotic strings.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.