Thursday, March 8, 2012

What makes Gauge-Transformations So Special

Gauge-Transformations are an arbitrary example of Gaussian Transformations.  Gauge-Transformations happen when electromagnetic energy scatters.  Gauge-Transformations are what in general produces entropy.  The physical activity that differentiates gauge-transformations from other Gaussian Transformations is that, during a gauge-transformation, not only do superstrings "shake" from within an eigenstate of the Klein Bottle, yet, the holonomic entity of the said Klein Bottle eigenstate here shakes through the Lagrangian of a bilateral coniaxial that may be mapped in a Laplacian manner at the center of the conipoint of the said holonomic entity of the said Klein Bottle eigenstate.  Yet, with other Gaussian Transformations, as the superstrings that "skake", so as to reattain the permittivity that these need to be discrete energy, from within a here given arbitrary Klein Bottle eigenstate, the holonomic entity of the here mentioned Klein Bottle eigenstate remains covariantly stationary per each metric in which the correlative superstrings that are here reattaining permittivity are "shook" so as to regain the said permittivity that these need so that the related superstrings may remain as discrete units of energy permittivity.  So, the individual eigenmetrics of Kaeler-Metric in gauge-transformations involve a bilateral wobble through a tightly-knit Lagrangian that may be mapped in the general locus of where the said Klein Bottle eigenstate is at during each of such described eigenmetrics, while the individual eigenmetrics of Kaeler-Metric in other Gaussian Transformations involve no covariantly viable shaking in the holonomic entity of the related Klein Bottle during the individual eigenmetrics that involve their respective Kaeler-Metric eigenstates.  The shaking of the given Klein Bottle eigenstates that happens during gauge-transformations produces an anharmonic shift in loci of Rarita Structure eigenstates that causes enough lack of discrete order so as to allow for those perturbations that cause the potentially needed reorganizations of the related Campbell, Hausendorf, and Campbell-Hausendorf Projections that increase the expectation value as to the ability of substringular subspaces to be able to maximize their agility in terms of their ability to help handle any given arbitrary alterations in norm-conditons.  These perturbations may spontaneously be needed so that the kinematic translations of norm-conditions, that may be necessary so that Fourier Transformations will not be bogged up, may be able to happen. Sincerely, Sam Roach.      

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