The Eleventh Session Of Course Ten

When a second-ordered light-cone-gauge topology is plucked by a gauge-boson, the activity of such plucking is known of as a light-cone related gauge-metric, and, the vibration of such a gauge-metric is known of as a second-ordered Schwinger Index.  The individual mini-string links between a superstring and its associated Fadeev-Popov-Trace are known of as second-ordered light-cone-gauge eigenstates.  The whole general holonomic field topology of these links that exist in-between a superstring and its corresponding Fadeev-Popov-Trace is known of as a first-ordered light-cone-guage eigenstate.  The sum of the vibrations that are formed by a first-ordered light-cone-guage eigenstate is known of as a Schwinger Index (first-ordered).  A second-ordered Schinger-Index may be delineated through an arbitrary given Rarita Structure eigenstate with a tense of orphoganal Yakawa gauge activity, and thus bear a harmonic wave propagation along the said associated Rarita Structure eigenstate.  Or, a second-ordered Schwinger-Index may be delineated with a tense of assymetric multiplicit (in terms of directorals) Yakawa gauge activity, and thus bear an anharmonic wave propagation along the same general type of associated Rarita Structure eigenstate.  When a gauge-boson (E(6)XE(6)) that plucks a second-ordered light-cone-gauge eigenstate does not bear a tense of borne tangency in terms of the associated homotopic Ward directoralization -- the gauge-boson as a whole is not orphoganal as a unit upon the given second-ordered light-cone-gauge eigenstate, the said  E(6)XE(6) string that forms the perturbation here in the proximal locus of the given arbitrary Rarita Structure eigenstate causes an anharmonic wave metric-gauge that, in and of itself, tends to move in the direction of the course of propagating an eventual Wick Action.  A Wick Aciton is the most important form of a Hausendorf Projection.