Part Two of Session 10 of Course 19 -- The Klein Bottle and Orbifold Differentiation

The protons of any given arbitrary atom, tend to be theoretically shaped in a basically parabolic manner -- when this is taken in a Laplacian-based manner.  For those atoms that work to bear the existence of neutrons as well, in the nucleus of the said respective atoms -- the so-stated neutrons, as well, also tend to be theoretically shaped in a basically parabolic manner -- again, when this is taken in a Laplacian-based manner.  If one were to spatially integrate one added so-eluded-to spatial parameter of orbit, to the dimensionality of the so-stated tendency of the nucleons of an atom -- that is, if one were to spatially integrate one Njenhuis-based tensor, in the form of an orbital-based coniaxion, to the spatial parameters of dimensionality of the said theoretical parabolic-based topological-based contour -- that is of the so-mentioned nucleons of any respective given arbitrary atomic structures, that have been eluded-to in this post, then, one would get a topological contour that would be of a four-dimensional spatial entity, that may here be described of as a genus of a set of given arbitrary multiplicitly taken F-field-based structures.  Such F-field-based structures that I have mentioned here, are described of in this respective given arbitrary case -- in terms of their differential clause as being in a timeless-based orientation.  This is due to the condition, that any holonomic substrate of topological-based phenomenology -- that exists in the form of an F-field, will bear a minimum of four spatial parameters of dimensionality -- in any minimum Fourier-based Transformation, in which such a so-stated F-field is differentiating in a kinematic manner, over time.  Any F-field that works to indicate the existence of a core-field-density, that is Gliossi to the directly corresponding holonomic structure, at the Poincaire level -- that would here consist of a set of superstrings, that operate in so as to perform one specific function, is an orbifold.  So, any respective given arbitrary proton, and, any respective given arbitrary neutron, when individually taken, exist as each working to bear the existence of being of an orbifold eigenset -- that will tend to exist at the general center, or, in other words, at the nucleus, of the respective atom -- in which such so-stated protons and so-stated neutrons are tending to be existing at -- over their correlative tense of a correlative Majorana-Weyl-Invariant-Mode.  (This is the tendency, in so long as their is not a directly appertaining mode of radioactive decay, that is then occurring to the directly appertaining atoms in question.)

I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.