FTAAN, Session 9

A point particle as it exists in a superstring has a core diameter of 5*10^(-87) meters. The mini-string that connects to these is 5*10^(-87) meters long. A mini-string has a thickness of 10^(-129) meters. These are taken in the substringular. In the globally distinguishable, these phenomena are 10^8*3 times thicker, since the Lorentz-Four-Contraction works to a factor of 3*10^8. So, in the substringular, the Lorentz-Four-Contractions are maximized for optimal core detection possible. Thus, in the substringular, one has minimal to no increased Lorentz-Four-Contraction. As a point particle of the first-order travels through ultimon flow the given point particle has mini-string taken away by means of it being pulled out of the bundle to where the given point particle has then 10,000 times less volume during the core of ultimon flow, since the associated bundle has less mini-string, although the bundle has the same diameter. The compactified condition of a point particle is densely configured. This densely volumed point during the core of ultimon flow differentiation by a factor of 10,000 to exist at the whole volume of its neighborhood by a certain number of times since the loose bundle discussed is relatively thinned out here. It does this by molding into different morphologies that total to its total volume of a first-ordered point particle a certain number of times within the core of ultimon flow. The volume normally taken up by a first-ordered point particle is known as a point particle neighborhood. A point particle of norm state during the ultimon flow has the volume of a first-ordered point particle of a string during the core of ultimon flow. A point particle of a norm state during BRST is just 50 times smaller in volume to a supersting's point particle during BRST. Point particles of superstrings of non-abelian superstrings are more loose than those of abelian supertrings.