Saturday, March 2, 2013

Another Look At the Cassimer Effect

It is a format of the ultimate fractal of pressurized vacuum, in the form that I term of as sub-mini-string segments, that binds the third-ordered point particles and the second-ordered point particles in such a manner in so that the directly related mini-string may comprise the substringular fields that work to form the activities and the phenomenology of the substringular.  The space-hole is when homotopy almost breaks down so that the substringular arrangements may be mildly altered in-between the individual iterations of instanton so that Gaussian Transformations may persist so that phenomena may spontaneously and persistently interchange eigenstates so that energy may continue to exist at all.  The space-hole, then, has a lot to do with Cassimer Invariance.  Cassimer Invariance is the perpetual tendency of substringular phenomena interchanging eigenstates to maintain homotopy per instanton.  Cassimer Invariance is thus helped by the conditional basis of the activities that happen during the space-hole.  The space-hole is allowed to happen due to the fifth force that I term of as the format of the ultimate fractal of pressurized vacuum.  As many people know, the Cassimer Effect is related to the condition of a pressurized vacuum.  This works to correspond the activities of Cassimer Invariance to the Cassimer Effect.  If it wasn't for the activities of Cassimer Invariance, once one superstring became frayed, all substringular phenomena would become frayed.  Yet, Cassimer Invariance is an activity that happens naturally as a fact of the substringular phenomena in general.  Here is more of a detailed explanation as to how the activities of the space-hole happen.:  The Bases of Light are in the process of being physically eigen to their general environment right before the instanton-quaternionic-field-impulse-mode right before an iteration of group instanton.  Just as this is happening, superstrings of discrete energy permittivity are just a tad bit closer to their direct substringular counterparts then these are to be toward one another during a typical iteration of what these would be like during an instanton.  The structure of the topology of the Ward-Caucy bounds  of  the said superstrings and their counterparts starts to slack in the physical Neumman-Ward bounds that exists in between these two formats of general physical phenomenology.  Just as this just mentioned slack begins to happen, the general eigenstates of the eluded to general topological structural basis snaps back due to the pull of the "re-energized" format of the ultimate fractal of pressurized vacuum -- the sub-mini-string has an added sub-permittivity that works to pull the general topological structural basis that exists in-between the said superstrings of energy permittivity and their directly corresponding counterparts back together in a manner that works to re-assort the general loci of the substringular regions in such a manner that works to allow form certain changes in the eigenfields of what are to be the altered substringular neighborhoods -- in so that Gaussian Transformations may be facilitated to reformat into the needed changes in norm-conditions that are here needed so that energy may be covariantly kinematic in a codeterminable and in a codifferentiable manner that allows for multiplicit substringular interaction among the perpetually changing scenes in the substringular.  Just as the condition of homotopy snaps back into what may be termed of as a definitively safe manner, the activity of such snapping works to pull the substringular encoders in toward each other in their region -- in such a manner that pulls upon the world-tube portions of space-time-fabric -- so that the quaternionic-instanton-field-impulse is here underway.  Such a stated impulse "breaks the huddle" of the conditions that happens during what I term of as being existent during the overt general eigencondition of the Bases of Light and the overt general eigencondition of the space-hole, so that superstrings may be brought back into the conditions that are necessary for the ensuing eigenstate of group instanton.  I will continue with the suspense later!
Sincerely,
Samuel David Roach

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