Showing posts with label decompactifiication. Show all posts
Showing posts with label decompactifiication. Show all posts

Friday, June 17, 2016

Point Particle Diameter

Aside from what may happen due to both the indistinguishable replacement of the sub-mini-stringular allotment of the holonomic substrate of point particles, and also, aside from what may happen due to that fraying that may happen to the Fourier-based activity that happens often with the interaction of black-holes with point particles as well, a first-ordered point particle always has the diameter of a first-ordered point particle (10^(-86m)), a second-ordered point particle always has the diameter of a second-ordered point particle (10^(-129m)), and a third-ordered point particle always has the diameter of a third-ordered point particle (10^(-387m)).  Still, the scalar amplitude as the degree of the decompactification of a first-ordered point particle that works to comprise the Laplacian-based Ward-Neumman conditions of those first-ordered point particles that make-up the immediate topology of a superstring of discrete energy permittiviy, is of a factor of two, and, the scalar amplitude of the degree of the decompactification of a first-ordered point particle that works to comprise the make-up of the immediate topology of a point commutator -- is anywhere from a factor of just over two, to a factor of ten-thousand.  Point particles are diameter dependent -- as a contra-distinguishable condition that is often related to much larger phenomenology, which tend to be radially dependent instead.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.