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.
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