The Next Part of Session 8 of Course 19 -- The Klein Bottle and Orbifold Differentiation

If one were to majorize a basic sphere that had an added spatial parameter of dimensionality, of which would here directly appertain to the addition of a tensoric orbital axion, as a given arbitrary postulate of what could exist in this given case in the substringular -- one would then have here, in this arbitrary case, a sphere that could then exist as appertaining to it then bearing two additional tensoric axions -- in the form of a physically extrapolated space, that could here have a spatial orientation that would have an added tensoric spinor-based axion and an added tensoric radial-based axion, that would then be ammended to the originally mentioned orbital-based sphere of the said initial conditions of this respective given arbitrary case scenario.  If, instead, one were to majorize a sphere that had two initially added spatial parameters of dimensionality, of which would here directly appertain to the initial existence in this respective given arbitrary case of both a tensoric orbital-based axion and a tensoric spinor-based axion -- one could then get, as a resultant extrapolation -- a sphere that would then work to bear the then Gliossi-based presence of both a tensoric orbital-based axion, a tensoric spinor-based axion, a tensoric radial-based axion, and, as well, the presence of a transversel-base axion, with the latter two of such tensoric axions being made present by the process of the just mentioned process of the majorization of the so-stated initial postulation, that was here implied in the earlier part of this sentence. These last two posts of which elude-to the substringular existence of ten spatial dimensions plus time for photons -- as existent in any respective given arbitrary p-field -- of which woulf then be the minimal number of spatial dimensions that would exist for small particles that would then tend to move in such a p-field, as would be the case in any actual limited Fourier-based Transformation in which any of such respective given arbitrary individually taken orbifold eigensets that would exist spatially in a p-field, would bear a directly corresponding existence in, over any alloted given arbitrary time, as such a so-eluded-to particle would then exist as such in the said p-field, as a general tendency in any of such respective given arbitrary case scenarios.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam.