A Little Bit About Second-Ordered-Light-Cone-Gauge Eigenstates

When a second-ordered-light-cone-gauge topology is plucked "like a harp"by a gauge-boson, such plucking is known as a light-cone related gauge-metric, and the vibration of such a gauge-metric is known 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 field of these links between a superstring and its correlative Fadeev-Popov-Trace is known as a first-ordered-light-cone-gauge eigenstate.  The sum of the vibrations that are formed by a first-ordered-light-cone gauge eigenstate is known as a Schwinger Index.  In certain cases, a second-ordered Schwinger Index may bear a tense of orphoganal Yakawa gauge activity, and thus this may bear a harmonic wave propagation along the associated Rarita Structure eigenstate.  Or, in a different scenario, a second-ordered Schwinger Index may be formed with a tense of assymetrically multiplicit (in terms of directorals) Yakawa gauge activity.  The prior activity thus bears an anharmonic wave propagation along the associated Rarita Structure eigenstate.  Gauge-Bosons are always Gliossi upon the second-ordered-light-cone-gauge eigenstaes when these pluck the implied field-indices.  So, in this sense, the said gauge-bosons always have a borne-tangency upon the described light-cone-gauge-eigenstates.  Yet, when a gauge-boson (which is an E(6)XE(6) string) that plucks a second-ordered light-cone-gauge eigenstate does not bear a tense of overall tangency in terms of its 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 plucking causes a field-wise homeomorphic yet interconnected torsion upon the said E(6)XE(6) string that forms a perturbation in the proximal locus of Rarita Structure eigenstate that 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 Projection.  This is because the condition of a lack of adherent norm-stability in the field of the light-cone-gauge indirectly causes a need for an alteration in the norm conditions of a given said locus -- thereby causing the need for a Gaussian Transformation.  The Wick Action is a form of a Hausendorf Projection. This happens to be the most important form of a Hausendorf Projection.  This is because the multiplicit Wick Action indirectly causes the multiplicit Higgs Action to be kinematic upon the multiplicit Klein Bottle so that the Kaeler-Metric may occur.  The Kaeler-Metric happens in a manner that allows for Gaussian Transformations to be able to occur. The Kaeler-Metric is the activity that causes superstrings to attain and reattain the permittivity that these need so that discrete energy may exist and persist.  I will continue with the suspence later!  Sincerely, Sam.