Point particles

The Importance of Point Particles to the Existence of Superstrings

In order for superstrings to be able to differentiate and interchange kinematically, there must be point particles that are smaller than these discussed superstrings. A superstring has a length, for 1-D strings, and a circumference, for 2-D strings, of 3*10^(-35) meters in the globally distinguishable. When in a totally contracted state, such a scalar is 10^(-43) meters. A first-ordered-point-particle has a diameter of 10^(-86) meters in the substringular when including the Gliossi Field that is directly associated and thus comprises the said point particle. First-Ordered-Point-Particles are comprised of the substance of the field of superstrings, or, in other words, mini-strings. Mini-String is comprised of second-ordered-point-particles that exist adjacent to each other in exterialy bound "chains" of phenomena that are interconnected by third-ordered-point particles that are bound by sub-mini-string. Second-Ordered-Point-Particles are 10^(-129) meters in diameter in the substringular, third-ordered-point-particles are 10^(-384) meters in diameter in the substringular, and sub-mini-string is 10^(-1152) meters in diameter in the substringular. Sub-Mini-String is the smallest phenomena that is a thing while yet also a gauge-action. Third-Ordered-Point-Particles only exist where there are second-ordered-point-particles. Not only does sub-mini-string bind third-ordered-point-particles together, yet these also work to interconnect the second-ordered-point-particles that comprise mini-string. A physical entity that is smaller than a superstring is termed to be a gauge-action. So how does such a tying of fabric rety while yet maintaining homotopy? The "space-hole" is what I call the duration right before Instanton-Quaternionic-Impulse-Mode, which is right before instanton, which is when homotopy just begins to undue to allow any essential retying of string, yet, to such a minor amount that homotopy during successive instantons is maintained except for when it is frayed in a black-hole. Such a resewing of substringular phenomena is brought back into a multiplicitly discrete homotopy due to the pressure that is impelled upon adjacent superstrings due to the equal and opposite wave-tug of point-particles that acts Gliossi upon the said superstrings to just enough of an extent so as to snap the temporarily untying topology described back into a unified multiplicit homotopic topology.