More About the Activity of the Schwinger Indices

Gauge-Bosons pluck second-ordered light-cone-gauge eigenstates to form second-ordered Schwinger Indices.  The just mentioned Schwinger Indices exist as vibratory eigenstates that propagate along the Rarita Structure while also propagating along the topological region of the multiplicit Real Reimmanian Plane eigenregions where discrete units of energy permittivity and discrete units of energy impedance interact via mini-string (the mini-string of which is the field eigenstates of superstrings, the field eigenstates of the associated counterstrings, and the field eigenstates of the Fadeev-Popov-Traces that act as the inverse field trajectory of the just mentioned superstrings) to work toward the periodicity of the Kaeler-Metric via the activation of a Hausendorf Projection known of as the Wick Action.            
The vibratory oscillations which are comprised of second-ordered Schwinger Indices that allow for both the Laplacian and Fourier spin-orbital conditions of both orbifolds and orbifold eigensets cause those harmonic and anharmonic wave-tug conditions among substringular phenomena that allow for the spontaneous changes that are necessary so that the norm-conditions that exist among superstrings may, for the most part, be orientable in such a balance so that only a strong exterior force would otherwise be able to cause a disorientation in the prior mentioned general type of conditions.  Since the Rarita Structure eigenstates bear their covariant orientation between superstrings and particles that act as discrete units of gravity, and also while the vibrations that exist among both superstrings, orbifolds, and orbifold eigensets is synchronized by the tempering of Schwinger Indices with the topological Fourier activity of the substance that comprises substringular discrete energy along with the membranous phenomena that these exist in, this causes such a substringular conformity that fascillitates the ongoing existance of the covariantly kinematic norm-conditions which are to continue as these perturbate so that continued exist may occur.  When a Gaussian Transformation is thus necessary so as to allow the necessary alterations that are necessary so that the covariance of norm-conditions may be kinematic as described before, the Wick Action is thence pulled out as a Yakawa-Based natural response to such a need.  This here indirectly -- after more steps that I will not describe here -- cause Gaussian Transformations to occur.  Whenever there is a Gaussian Transformation, there is a sequential set of instantons that involves the Kaeler Metric.  The most common form of Gaussian Transformation is known of as a gauge-metric.