When a substringular cohomology reverses in its directoral-based holomorphicity, there is a reversal in the applicable Kaeler conditions, and, this works to form a Wick Action eigenstate -- of which works to initiate the process of a Gaussian Transformation, which involves the activity of a Kaeler-Metric eigenstate. When this happens, the directly corresponding gauge-bosons reverse in their holomophic-directoral basis. What this means, is that the gauge-bosons will here go from "plucking" their respective second-ordered light-cone-gauge eigenstates from one Laplacian-based direction of wave-tug/wave-pull -- to "plucking' their respective second-ordered light-cone-gauge eigenstates in the opposite Laplacian-based direction of wave-tug/wave-pull. When such a Gaussian Transformation here involves the scattering of electromagnetic energy, this is called a gauge-transformation. In relation to the gauge-bosons, this works to not only reverse the basis of their correlative holomorphic directoral tense, yet, it also works to reverse the parity of the vibrations that are formed by their plucking of their correlative second-ordered light-cone-gauge eigenstates -- the directly corresponding second-ordered Schwinger-Indices are here then reversed in the arrangement of their indical-based holonomic substrate. This is a beginning of an explanation as to the relationship between the activity of a gauge-transformation -- with the activity of the correlative gauge-bosons, that are here of the same respective given arbitrary basis of phenomenology.
To Be Continued! I will continue with the suspense later! Sam.
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