An Interim In-Between Sessions 7 and 8 of Course 19 -- The Klein Bottle and Orbifold Differentiation

Let us say that we are here discussing a bosonic superstring of discrete energy permittivity, that is of an orbifold eigenset -- that is differentiating in a kinematic nature -- at group-related instanton.  The said given arbitrary orbifold eigenset -- as each of the superstrings that work to comprise the respective orbifold eigenset -- is of a bosonic sub-atomic nature, to where the so-stated orbifold eigenset works to bear the nature as to having a whole spin, over any correlatively corresponding sequential series of affiliated group-related instantons, in which such a set of bosonic superstrings is of the so-stated substringular nature.  Since the orbifold eigenset that is being describe of here is entirely comprised of superstrings that are of a bosonic nature, each of the superstrings that would here work to comprise the said orbifold eigenset, would work to bear a whole spin, over the course of each individually taken iteration of BRST that is affiliated with the directly corresponding iterations of the said group-related instantons that are here to be considered.  This would be affiliated with the condition -- that each of the individually taken superstrings of discrete energy permittivity that would here work to comprise the so-stated orbifold eigenset of this respective given arbitrary case, would tend to oscillate in a harmonic nature, during the course of each individually taken iteration of BRST -- that is here directly affiliated with the correlative iterations of group-related instanton -- in which both the constituent superstrings and the orbifold eigenset that these substringular members work to make-up is active as a Hamiltonian operator, that is to perform one given arbitrary function in the substringular, over time.  Since the so-eluded-to orbifold eigenset of this given arbitrary case is here comprised of superstrings that are tending to oscillate in a harmonic manner during each individually taken iteration of BRST, then, the individually taken partials that would here work to comprise the Hodge-based fractals of the discrete energy -- that would work to comprise the sum of the discrete quantum of energy, that each of such superstrings works to make-up -- would then tend to bear a higher probability of working to bear a relatively unitary directoral-based flow of angular momentum-based permittivity.  So, if such a tendency is to be incorporated into the overall flow of the directorial-based flow of the angular momentum-based permittivity of the directly associated orbifold eigenset of this case as well, then, there is here more of a likely-hood of there being less of a need for extra Klein Bottle eigenstates to be able to facilitate the activity of any potential proximal Kahler-Metric -- if such a Kahler-Metric is to then be needed to be performed by the substringular members that are in the set relative general locus in which such a so-stated respective given arbitrary orbifold eigenset is to be differentiating in in a kinematic nature, over the so-eluded-to correlaltive sequential series of instantons.  To Be Continued!  Sincerely, Sam Roach.