Part Two As To Why Gauge-Transformations Are Thus Called

When a superstring of discrete kinetic energy permittivity from an electron is to undergo the Fujikawa Coupling via the Green Function, in the process of being expelled from the said electron into the form of a photon, -- the correlative open string of discrete kinetic energy permittivity is to then to be transformed into a closed string of discrete electromagnetic energy permittivity over, the course of the so-eluded-to duration of such a correlative Fourier Transformation.  An open string is fermionic.  A closed string is bosonic.  Fermionic superstrings of discrete energy permittivity work to each bear five second-order light-cone-gauge eigenstates to work to comprise the one first-order light-cone-gauge eigenstate, that is to directly correspond to that respective given arbitrary fermionic superstring.  Bosonic superstrings of discrete energy permittivity work to each bear ten second-order light-cone-gauge eigenstates, to work to comprise the one first-order light-cone-gauge eigenstate that is to directly correspond to that respective given arbitrary bosonic superstring.  When the Fujikawa Coupling is to happen to one given arbitrary respective fermionic superstring as such, each of the five second-order light-cone-gauge eigenstates that had here to have worked to form primarily the wave-based quantum of the discrete energy impedance of the directly corroborative discrete quantum of energy bundle (via the net overall Schwinger-Index eigenstate that is to thus to be formed by those vibrations, that are here to be made by the "plucking" of the individually taken said second-order light-cone-gauge eigenstates), -- is to retie into ten second-order light-cone-gauge eigenstates, that are then to be of the discrete energy quantum bundle of the here resultant bosonic superstring as such.  The second-order light-cone-gauge eigenstates that are of a bosonic superstring of discrete energy permittivity, always tend to bear half of the cross-sectional thickness of the second-order light-cone-gauge eigenstates that are of a fermionic superstring of discrete energy permittivty.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.