More As to the Formation of Schwinger-Indices

Gauge-Bosons pull upon second-ordered light-cone-gauge eigenstates as these "pluck" the said eigenstates in such a manner in so that the said gauge-bosons are Gliossi to the eluded to second-ordered eigenstates, as the directly corresponding given arbitrary superstrings are initially swayed during BRST in the relatively forward-holomorphic direction, while, the said gauge-bosons are not Gliossi to the directly corresponding second-ordered light-cone-gauge eigenstates as the directly associated superstrings are swayed during BRST in the relatively reverse-holomorphic direction.  The moment of the eluded to release from the format of Gliossi-based Yakawa Coupling that was eluded to is during the completion of the eluded to relatively forward-holomorphic topological sway of superstrings -- right before the directly corresponding superstrings are swayed in a subtle manner in the respective relatively reverse-holomorphic directoral-based pull.  As the so-stated Gliossi-based tug that is operated by gauge-bosons is released, the corresponding vibrations that are Poincaire to the corelative second-ordered light-cone-gauge eigenstates are put into kinetic motion in the form of second-ordered Schwinger-Indices.  The integral effect of the interaction of the second-ordered Schwinger-Indices that stem from a whole first-ordered light-cone-gauge eigestate is what may be termed of as a first-ordered Schwinger-Index.  I will continue with the suspense later!  Sincerely, Samuel David Roach.