A Tad Bit Of An In-Depth Discussion

A field that is tachyonic is a perturbative field that becomes divergent from an initial state of a relative tense of conformal invariance -- or, from an initial condition of Noether Flow -- into a flow that involves a combined Real and Njenhuis given arbitrary format of tensors that work to inter-bind the eluded to phenomenon that here becomes tachyonic. This process ends-up resettling the said phenomenon at a relatively distant locus, in a manner that involves a format of a re-convergence back into Noether Flow, once such a phenomenon settles, for the said phenomenon that had here become tachyonic previously. Either way, any tachyonic field will end-up forming a Wick Action eigenstate in so as to produce an ensuing Gaussian Transformation. So, any tachyonic field will involve a Cambell-Hausnedorf-Projection eigenstate that will pull upon a Hausendorf-Projection known of as a Wick Action eigenstate --  in a manner that acts as a correlary to the genus of activity that pulls a Wick Action eigenstate into a Landau-Gisner-Action eigenstate -- due to the indirect influence of the directly associated light-cone-gauge eigenstates upon the local Rarita Structure, as a given arbitrary phenomenon is acting in a tachyonic manner. The said Landau-Gisner-Action eigenstate then acts upon a Campbell-norm-state that works to physically leverage a Klein Bottle eigenstate via a holonomic substrate known of as a Higgs Boson eigenstate, in so as to pull the just mentioned Klein Bottle eigenstate into the general locus in which certain given arbitrary superstrings that need to undergo a Kaeler-Metric eigenmetric may be able to do so.  The Kaeler-Metric is the duration in which superstrings are differentiated upon in such a manner to where these corresponding superstrings may be able to undergo a Gaussian Transformation.  The format of the manner as to how the Klein Bottle eigenstates are put together is called the Schotky Construction.  When the Ward-Caucy-based plane of superstrings that are to enter a Klein Bottle eigenstate falls into the said Klein Bottle in a hermitian manner (in a flush manner), then, the directly related Gaussian Transformation is not a gauge-transformation.  So, when the Ward-Caucy-basd plane of superstrings that are to enter a Klein Bottle eigenstate bears Chern-Simmons singularities upon entry to the respective Schotky Construction (when the eluded to entry is not flush), then, the directly related Gaussian Transformtion is a gauge-transformation.  Another way of looking it is, when a Klein Bottle eigenstate is relatively stationary or static during a sub-metric of a directly related Kaeler-Metric, then, the directly related Gaussian Transformation is not a gauge-transformation.  Yet, when a Klein Bottle eigenstate wobbles at all beyond its basic static core vibration, then, the directly related Gaussian Transformation is a gauge-transformation.  The need for gauge-transformations when E.M. scatters is one given arbitrary case of such an activity. (Although light that scatters moves slower than in a vacuum, on the whole.) The activity of gauge-transformations not only allows for those Gaussian Transformations that involves that re-assortment that is necessary for E.M. to be propagated without disruption, yet, such activity also, ironically enough, works to allow for for the creation of entropy. Entropy is needed for the neccesary changes in physical states. To Be Continued! Sam Roach.