About the Transference of Third-Ordered Schwinger Indices

So, how do third-ordered Schwinger Indices become taken out of their directly corresponding respective light-cone-gauge eigenstates -- into the general Ward-Caucy bounds of the directly correlative Rarita Structure eigenstates?  Let me start to explain this here.  Initially, the gauge-bosons of the second-ordered light-cone-gauge eigenstates that work to comprise one unique respective given arbitrary first-ordered light-cone-gauge eigenstate "pluck" the here so-eluded-to second-ordered light-cone-gauge eigenstates, in so as to form the three-hundred third-ordered Schwinger Indices that would here be directly corresponding to the operational Hodge-based interplay of the here mentioned and eluded-to first-ordered light-cone-gauge eigenstate, that works to form the wave-functionability of the discrete energy impedance of one discrete unit of energy in time and space.  During the first six hbar increments of one iteration of group instanton -- of which would here directly correspond to the gauge-metrical activity that happens during one unit of BRST -- the so-stated "plucking" of the second-ordered light-cone-gauge eigenstates works to form third-ordered Shwinger Indices that start to vibrate at their general loci along the topology of the holonomic substrate of the said light-cone-gauge eigenstates.   These just eluded-to vibrational oscillations that work to perturbate the just mentioned eigenstates of the wavefunctionability of discrete energy impedance, immediately upon virtual resonation, are pulled by core-field density -- in a general directoral wave-pull, that is directed outward from the general locus of the here respective Ward-Neumman bounds of the directly correlative first-ordered light-cone-gauge, that is directly associated with the substringular holonomic substrate of discrete energy of the so-eluded-to general locus.  Right at the point that the initial 6 hbar increments of Real Reimmanian-based time of the correlative iteration of the corresponding instanton have elapsed, the so-stated third-ordered Schwinger Indices have reached the relative exterior of the Ward-Neumman bounds of the directly corresponding first-ordered light-cone-gauge-based substringular neighborhood.  This is simultaneous -- as is according to the vantage-point of a central conipoint -- to when the very end of BRST has just come to completion.  This is, as well, simultaneous -- as is according to the same just mentioned vantage point (of a central conipoint) -- to the ending of both the Polyakov Action and the Bette Action of the directly corresponding discrete energy of this case, at the so-mentioned specific locus at hand.  So, for the last (2pi-6) hbar increment of Real-based time, for the so-stated third-ordered Schwinger Indices, these vibrational oscillation-based indices are then made to inact a relatively high projected kinematic-based torsioning upon the surrounding Rarita Structure eigenstates -- over the course of the very ending of the directly corresponding duration of such a case of group-instanton -- in so as to work, per each successive iteration of instanton, at forming a sequential series of interactions of discrete energy upon gravitational-based strings, over time.  This is part of as to why we, as humans, tend to only perceive of the instant that happens right at the ending of BRST.  This works in so as to form that scalar attribute of the Rarita Structure eigenstates upon superstrings of discrete energy -- in the process of working to make what is known of as the Ricci Scalar to take effect, so that  there may be a covariant, codeterminable, and a codifferentiable manner as to the relationship between discrete energy and gravity itself.
To Be Continued!  Sam Roach.