Tuesday, March 13, 2012

More About The Manner Of Gauge Transformations

As the concept was mentioned before, the basic difference between gauge transformations and other Gaussian Transformations is a matter of the wobble of the Klein Bottle during the sub-metrical duration during the end of instanton after BRST in which the activity of the Kaeler-Metric is kinematically Gliossi upon those superstrings that here need to reattain permittivity so that these may remain as discrete energy permittivity.  The general manner as to what physically goes on during a Gaussian Transformation that is not a gauge transformation was discussed yesterday.  Now, I will discuss what physically goes on during a gauge transformation.  (Gauge Transformations are arbitrary examples of Gaussian Transformations.)
During any Gaussian Transformation, the norm conditions that exist in a set locus are undergoing changes in their differentially geometric delineation so that covariant redistribution of related superstrings may happen so that motion may persist period.  Gauge Transformations are Gaussian Transformations that involve the reverse fractal process of the scattering of electromagnetic energy, which, thus, involves the creation of entropy that is at least needed so that there may be changes in physical states of molecules and other compounds.  The wobble of the related multiplicit Klein Bottle eigenstates that happens during the kinematic import of the Kaeler-Metric eigenstates during gauge transformations is caused by the change in the abelian nature of the phenomena that changes in terms of light-cone-gauge topology during the said gauge transformations.  When electromagnetic energy scatters upon anything, it initially alters from having a non-abelian to an abelian light-cone-gauge topology -- while soon later converting back to having a non-abelian light-cone-gauge topology.  Such a change from a Yang-Mills to a Kaluza-Klein and back to a Yang-Mills topology produces a temporarily relaxed substringular field that interconnects multiplicitly to a given arbitrary set of Klein Bottle eigenstates that subsequently retightens in terms of the sway of the elastic modulae of the mini-string that binds at the conipoints of the coniaxials where the given Klein Bottle eigenstates are most directly physically bound to the Rarita Structure when the Kaeler-Metric happens in a general locus.  Such an activity causes the substringular field that binds any Klein Bottle eigenstate to change from being abelian to non-abelian and back to abelian in terms of the differential geometry that acts as a collary to the light-cone-gauge topology alteration that happens to those photons whose scattering causes the related gauge transformation to happen.This is what causes the related Klein Bottle eigenstate to sway one Planck Length forward holomorphically while simultaneously one Planck Radial norm-to-forward-holomorphically to back to its original state while then swaying one Planck Length antiholomorphically and simultaneously one Planck Radial norm-to-reverse-holomorphically to back to its original state during the sub-metric that occurs during one eigenstate in which the Kaeler-Metric is kinematically Gliossi upon the superstrings that are shook in the Klein Bottle during the said sub-metric.  Since such an activity tends to disorient superstrings, such an activity temporarily causes a very temporary conditon of certain involved superstrings to be tachyonic, while also causing the creation and persistence of entropy.  Here, the disorientation of the related superstrings here is generally only handled during the succeeding Regge Action eigenstates that relate to the corresponding Klein Bottle eigenstates that involve gauge-metric eigenloci where the scattering of EME is scattered.  Go To Run!  Sam.            

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