Part Three of Session 9 of Course 18

When one is dealing with first-ordered point particles in the substringular, one is dealing with condensed oscillation of mini-string or condensed oscillation of core-substringular-field-density -- that would here come together in a form that one may say acts like a  "ball of yarn" of the just-mentioned condensed oscillation -- in so as to form a given arbitrary degree of a compactification of the so-stated local multiplicitly torsioned core-field density, in so as to form one immediate eigenmember basis of what may be either termed of as a point commutator that would here work to form a superstring, or as a point commutator that would here work to form a superstringular counterpart.  So, when one is dealing with the extension of mini-stringular segments that are jutted-out from any given first-ordered point particle, that would here work to form a ground-based superstring of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out from the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point particles that work to form the same respective directly associated given arbitrary superstring, and, to the most adjacent first-ordered point particle of the directly corresponding counterstring of discrete energy permittiivity -- one is then  here working with only one of such jutted-out mini-stringular segments.  Yet, when one is, instead, dealing with the extension of mini-stringular segments that are jutted-out from any given arbitrary first-ordered point particle, that would here work to form a Fock-based superstringular counterpart of the wave-functionablitiy of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out form the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point partictles that work to form the same respective directly associated given arbitrary counterstring, and, to the most adjacent first-ordered point particle of the directly associated superstring of discrete energy permititivity  -- one is then here working with many of such jutted-out mini-stringular segments.  The orientation of any given arbitrary first-ordered point particle to its surroundings, where it is positioned in its neighborhood, and, the pointal localization of the said point -- when this is taken relative to its environment -- is the basis for a respective fractal of electric field.  The coordinates that make it a field are the single wave propagations that are extended from the just so-eluded-to substringular neighborhoods.  To Be Continued!  Sam.