Monday, September 3, 2018

Important Stuff About The Kahler-Metric

Here's the difference between the general condition of a given arbitrary superstring of discrete energy permittivity being just Yukawa to the Kahler-Metric, versus such a superstring to, instead, to be Gliosis to the Kahler-Metric.  Any superstring of discrete energy permittivity that is unfrayed, will always be Yukawa to the Kahler-Metric -- since a superstring being Yukawa to the Kahler-Metric, is directly appertaining to those dimensional-based propensities, that are appertaining to the conditions of a pulsating discrete increment of energy.  Yet -- what I name of as being GLIOSIS to the Kahler-Metric, is when a discrete quantum or a set of discrete quanta of energy, work to interact with what I will name, for brevity's sake, the "Klein Bottle Apparatus," in such a manner, not only to where such a dimensional-based propensity of pulsating discrete energy may both persist and exist over time, yet also, in so as to work to allow for such an ealier said dimensional-based propensity to be able to both persist and exist over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

No comments: