Beads Of Particles

What I term of as being mini-stringular segmentation -- is that inter-connective bead, that is comprised of what I term of as being second-order point particles, that exists in such a manner, in so as to come together with the multiplicit phenomenology of all of rest of such segmental entities, in a way that tends to be pervasive -- all along the arena of the substringular, -- in so as to work to inter-connect that general field, by which the Ward-Cauchy-based conditions of homotopy may transpire.  Likewise -- when such a general tendency is here to be taken at a reverse-fractal level -- each superstring, as is according to my model of string theory, is comprised of a bead of first-order point particles. Sam Roach.

A Little About The Size Of Certain Phenomena In The Substringular

Let us consider differential operators that are based on exact and linear associations of points from within their neighborhoods. If the points form exact differential associations, then these are 3*10^(-78) meter apart in the globally distinguishable and 10^(-86) meter apart in the substringular. If a differential association of points is linear, then you may draw a straight line from one end of the association to the other. Generally, a set number of points from strings come together at the center of state of each tori. These points then get "picked up" by constituent-force-sectors that tend to remain in the "line of fire" of these center of state points from strings. The forward time momenta related points then travel counterclockwise around our space-time-continuum to the tori sector region right before the prior tori sector region. The points then travel down the heterotic string, across, and up to the parallel tori sector region of the middle-continuum. The forward time momenta related points then travel counterclockwise to the tori sector region right before the prior tori sector region. The points then travel down the heterotic string, across, and up to the parallel tori sector region of the far-continuum. The forward time momenta related points then travel counterclockwise to the tori sector region right after the prior tori sector region. The points then travel down the heterotic string, across, and up to the parallel tori sector region of the middle-continuum. The forward time momenta related points then travel counterclockwise to the tori sector region right after the prior tori sector region. The points then travel down the heterotic string, across, and up to the parallel tori sector region of the near-continuum (where we live). The forward time momenta related points then travel counterclockwise a little more than one rotation of the our space-time-continuum to the tori sector right after the prior tori sector region. The five thousand substringular encoder templates and the five thousand substringular counterstring templates of the given tori sector then have begun a momentary breach of topology that is brought together by mini-strings (10^(-129)meter thick). This temporary breach is called the "space-hole." Once the "space-hole" happens, the quaternionic-instanton-impulse pulls the substringular templates and the substringular counterstring templates into the heart of the given tori sector region so that the substringular may reiterate. At this time, the globally distinguishable time of 10^(-43)second happens. The substringular pulse in-between globally distinguishable time is 10^(-43)second (H time).

                       
The "space-hole" is for about .283 H bar tme in the substringular.

We only notice globally distinguishable time.

Please tell me what you think of this!!!

Remember, be as tough as a fiber that is 3*10^(-35) meter long!

Catch you two! (Peace)

Sincerely,

Samuel Roach
                         
               

FTAAN, Session 10

A superstring has point particle cores that are 5*10^(-87) meters thick in the substringular and 1.5*10^(-78) meters thick in the globally distinguishable. The mini-strings in-between these are 5*10^(-87) meters long. So, above the top point particle of the first order of a one-dimensional superstring is an antenna-like profection of mini-string that is often non-abelian in and of itself per iteration, whether the given superstring is abelian on the whole or non-abelian on the whole. When a two-dimensional non-abelian superstring of a non-swivel nature iterates, the mini-strings in-between the given first-ordered point particles vibrate holomophically/antiholomorphically 60 times each without moving the given first-ordered point particles during the core of BRST. When a one-dimensional non-abelian superstring of a non-swivel nature iterates, the mini-strings in-between the given first-ordered point-particles vibrate norm to holomorphically and norm to the Lagrangian of the substance of the superstring/norm to antihlolomorphically and norm to the Lagrangian of the substance of the superstring 60 times each without moving the given first-ordered point particles during the core of BRST. When a one-dimensional abelian string iterates mini-string ripples through the first-ordered point particles causing the mini-string in-between these to begin to kink at their center states sixty times norm to the holomorphic yet also norm to the Lagrangian substance of the superstring and sixty times norm to the antiholomorphic yet also norm to the Lagrangian substance of the superstring without moving the given first-ordered point particles during the core of BRST because the given ripple of the mini-string of the first-ordered point particles provides phenomena to the mini-string. When a two-dimensional abelian superstring iterates, the same thing happens except that the mini-string vibration kinks the mini-string 60 times holomorphically and 60 times antiholomorphically. The vibration of non-abelian strings and the kinks of abelian strings happen holomorphically then antiholomorphically back and forth, or norm to these and the Lagrangian of their substringular substance back-and-forth. This happens without moving the core of the first-ordered point particles during BRST.