As To The Striking Of Light-Cone-Gauge Eigenstates

When any given arbitrary gauge-boson acts to initially start to "pluck" a second-order light-cone-gauge eigenstate during BRST -- the initial contact works to tend to form metrical Chern-Simmons singularities, proximal to the specific locus that is Poincare to the Gloisis area of contact.  Right after the so-stated gauge-boson is done pulling upon the specific locus where the said plucking is metrical in operation -- the metrical singularities that are formed at the specific locus where the then formed Schwinger-Index is initiated, are then no longer of a Chern-Simmons nature --, these singularities are, at this duration-based point, tending to be of a hermitian nature -- over the course of this said gauge-metrical activity.  This is the tendency of the case, whether the resultant Schwinger-Index is of a harmonic or of an anharmonic nature -- as such said Schwinger-Indices are then propagated from the general locus of the light-cone-gauge, outward and along the Rarita Structure.  Here:  Gauge-Bosons are of the nature as to being considered as E(6)XE(6) strings.  These said strings are a genus of a heterotic string. As such a heterotic string initially contacts a specific locus of a second-order light-cone-gauge eigenstates -- this will tend to form spurious gauge-metrical pulsation, that are of either a dampened nature or of an elongated nature.  Once the pull of the so-stated gauge-bosons is released -- the vibrational oscillation of the topological fabric of the said second-order eigenstate of the wave-functionabilty of discrete energy impedance, is pulled into a manner that tends to work at utilizing the initial said spurious pulsations that are Poincare to the locus of the said plucking,--  in such a manner in so as to work to form either a harmonic or an anharmonic wave-pulse transfer of the so-eluded-to disturbance in space -- to where the then initially formed vibrational oscillation will then tend to bear a tense of hermitian singularities -- to where the then initiated wave-based propagation may be pulled into the Rarita Structure, in so as to work at forming the needed interdependent operations that these have in the substringular.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.