Friday, December 5, 2014

Part Four of the Fourth Session of Course 18

After succeeding iterations of group instanton, the spatial relationships between any given arbitrary superstring of discrete energy permittivity and its directly corresponding counterstring tends to alter -- in one manner or another.  If any given arbitrary superstring of discrete energy permittivity and its counterpart are not orientable during one or more of the just mentioned successive iterations of group instanton, and also, if the same so-stated superstring and its counterpart are -- at this metrical point in time -- not orientable during the correlative iterations of one or more Regge Action eigenmetrics, then, such a superstring that I have been discussing here will not be orientable -- which will work to indicate the characteristic as to that the said superstring will be tachyonic during the immediately following iteration of group instanton, once again, when the so-eluded-to superstring is not orientable during both the Bette Action eigenmetric and its correlative Regge Action eigenmetric, that would here appertain to the same singular iteration of group instanton.  Generally, though, any given superstring and its correlative counterstring will tend to be renormalizable -- as may be denoted by the condition that superstrings tend to move as is according to Noether Flow.  Yet, if a superstring and its correlative counterstring were always normalizable -- with not chance for tachyonic flow at all -- the eigenbase of all substringular activity would spontaneously become of a static-based nature, which would work to eventually end the activity of energy, over time.   This works to indicate the need for at least a certain degree of tachyonic flow, in order for energy to be perminently existent.  Yet, because of what may be termed of as the Bette Field Transformation, observable activity is conditioned to be of a perminantly existent nature, over time.  Bette Field Transformations may often, though, in one specific general locus or another, be of a superconformal nature, when the energy at a relatively limited set locus is conditioned to be in a tense of static equilibrium.  Also, often, Bette Field Transformations may be of a conformally invariant nature that is not superconformal -- when one is here dealing with a harmonic-based system that operates in a manner that works to form  Hamiltonian-based field-indices that may be denoted as bearing an extrapolatable manner of viabely detectable re-delineation, over time.  Yet, also, a Bette Field Transformation may be of a divergent nature -- when the correlative substringular activity is perturbative -- to where the activity that is here denoted is perminently scattered from a relatively speaking general locus.  To Be Continued!  Sam.
 I will continue with the suspense later!!!

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