Part Two of As To the Fractal of Electric Current

Now, let us examine the nature of a pointal-based phenomenology, in general, in light of what may be termed of as the Pauli Exclustion Principle.  As according to what may be eluded-to by the Pauli Exclusion Principle, phenomena can not be at the very same spot at the very same time.  More literally, the Pauli Exclusion Principle amounts to the condition that two adjacent electrons will always tend to bear asymmetric spins -- when such spinning is related to the one here respective given arbitrary electron as taken relative to the other adjacent here respective given arbitrary electron of such a just eluded-to case scenario.  Furthermore, as to the spin-based nature of first-ordered point particles (those point particles that are of one genus of scalar magnitude-based size smaller than superstrings of discrete energy permittivity) is to where the relative "neighborhoods" of the said superstrings tends to remain constant over time -- in so long as the directly corresponding superstring remains unfrayed in topological-based homotopic condition, -- yet, the specific delineations of the multiplicit substringular neighborhoods of the so-stated first-ordered point particles may often be quite variable from one iteration of group instanton where these point particles are exemplified, to the next of such instantons.  For instance, let us here consider a two-dimensional superstring that is accelerated from a terrestrial-based rest up to a velocity that is contingent upon what causes the said two-dimensional superstring its maximum-based Lorentz-Four-Contraction that a non-electromagnetic-based superstring may possibly bear.  As the so-eluded-to Lorentz-Four-Contraction is brought from a factor of one to a factor of three million, the directly corresponding superstring that is involved with the so-stated first-ordered point particles is shortened in circumference and length by a factor of three-hundred-million.  In the process, although the superstring that is here directly associated is shortened by a factor of three-hundred-million, the size of the directly associated point particle neighborhoods are not changed at all -- in so long as the contingent superstring is to be unfrayed.  Its just that the directly corresponding core-field-density or mini-stirng that works to bind the affiliated superstring, as the so-stated string becomes more and more contracted, is brought to where there is less and less of a separation between the said directly associated first-ordered point particles in the course of the said Lorentz-Four-Contractions.