Part Six of Session Three of Course 19 -- The Klein Bottle and Orbifold Differentiation

Those Wilson Lines -- that would here directly appertain to the basis of the composition of any respective given arbitrary Klein Bottle eigenstate, tend to behave, in part, like "limp shades" that may often be penetrated by an external force, over a successive series of instantons.  So, as a relatively stable Klein Bottle-related construction works to wobble in any given arbitrary Minkowski-based directoral combination  that includes up to a total of six Njenhuis additional spatial dimensions -- over the course of a tightly-bound Fourier-based translation of the here directly pertinent substringular members -- that would be local to the motion of the here respective given arbitrary Klein Bottle eigenstate of this specific case scenario, those external-based tensoric-related Hamiltonian operators that are to here interact with the said Klein Bottle eigenstate in an acutely Yakawa manner, will here bear a relatively non abelian-based wave-tug/wave-pull upon the so-stated Klein Bottle eigenstate of this case.  This so-eluded-to Njenhuis eigenbase of topological sway, of which is local to a set of tensors that are off of the Real Reimmanian Plane, will tend to be more limited at working to pull or tug at the construction of the said respective given arbitrary Klein Bottle eigenstate.  This tendency is on account of the condition that the so-eluded-to holonomic structure --that is here to bear the said Njenhuis eigenbase of a relatively non abelian wave-tug/wave-pull, that is projected at a relative distance upon the Gliossi-based phenomenology of the so-stated Klein Bottle eigenstate, would here be locally proximal to a substringular neighborhood that is then here situated off of the relatively Real Reimmanian Plane.  It would then follow here, that the directly corresponding cohomological eigenbase of that phenomenology -- that would here be applying the Njenhuis topological sway upon the said Klein Bottle eigenstate -- will here tend to bear a higher scalar degree of a Ricci Scalar-based index that is then of a Doubolt cohomology, than that phenomenology that would, instead, be more directly related to that cohomological framework that is directly corresponding to the physical memory that would here be formed by the holonomic substrate of the said respective given arbitrary Klein Bottle eigenstate of such a case,itself.
To Be Continued! I will continue with the suspense later!  Sincerely, Sam Roach.