Session 12 of Course 13, Part one

There are differences between a superstring and a counterstring.  Here, we will compare the differences between a superstring of discrete energy -- that exists in one set of world-tubes -- and its counterstring.  A one-dimensional superstring is ideally a basically straight strand of first-ordered point particles, with the exception from straightness being one or more partitions that exist interior to the ends of the said superstring's opposite Neumman bounds.  The said one or more partitions are first-ordered point particles that may be mapped over to the side of the general line of the given arbitrary stream of point particles by a static-based distance of the diameter of one first-ordered point particle.  Such point particles that I am referring to have the diameter of 10^(-86) meters in the substringular -- even though these may be extrapolated as having a diameter of 3*10^(-78) meters in the globally distinguishable, due to certain effects that happens to these particles during the Polyakov Action.  A one-dimensional superstring that is relatively ideal has a counterstring that has one or more partitions on the relatively opposite side of the string when relative to the given superstring.  The Grassman Constant of such a superstring/counterstring inter-relation is here the angle of difference that exists between the partitions of the said given one-dimensional superstring and the corresponding partitions of the one-dimensional counterstring.  A two-dimensional superstring is ideally a basic hoop of first-ordered point particles, with the exception from "perfect" roundness being partitions that work to allow for discrete permittivity -- just as with one-d superstrings.  Part two later!