Session 13 to Course 13

The substringular encoders encode for superstrings.  Substringular encoders attach to superstrings and their correlative Planck-like phenomena via mini-string-based stratum.  The holonomic topological substrate that substringular encoders work to encode for is branched-out from the directly related substrings of the substringular encoders over to the Planck-like phenomena.  The superstrings in their respective world-tubes -- along with the counterparts of the directly corresponding superstrings -- are attached to the Planck-like phenomena via the multiplicity light-cone-gauge eigenstates.  Substringular encoders each consist of 10^43 substrings that exist well off of any given arbitrary Real Reimmanian Plane in which both superstrings of discrete energy permittivity and gravitational particles differentiate directly in during any given arbitrary individual iteration of instanton.  Each substring of a substringular encoder is the same size and shape as a one-dimensional superstring that is relatively ideal, except that these encoder mers have no partitions in and of themselves.  So, a substringular encoder that is based on a bosonic or closed string pattern consists of 3*10^8 mers of substring that work to form an approximation of a hoop-like pattern that is relatively homeomorphic except for the exception of its partitions, while a substringular encoder that is based on a fermionic or open string pattern that is linearly-based except with the exception of its partitions.  Each substringular encoder that is of normal space has 10^39 partitions in so long that this substringular encoder does not cause a black-hole to form.  Substringular encoders that cause black-holes to form have 10^40 partitions each.  In a one-dimensional substringular encoder, partitions go from right to left, facing the counterclockwise Ultimon general direction.  In two-dimensional substringular encoders, partitions go from right to left while also from up to down -- facing the counterclockwise Ultimon direction.  Even though there more bosonic superstrings of discrete energy permittivity than fermionic superstrings of discrete energy permittivity, there are just as many one-dimensional substringular encoders as there are two-dimensional substringular encoders.  Each substringular encoder has a counterstring that exists in its forward-holomorphic-based direction at instanton.  The partitions of a one-dimensional substringular encoder counterstring go from left to right, facing the counterclockwise Ultimon direction.  The partitions of a two-dimensional substringular encoder counterstring go from left to right while also from down to up, facing the counterclockwise Ultimon direction.  The angle of difference between the partitions of a substringular encoder -- and the partitions of a substringular encoder counterstring -- is part of the conditional basis of another format of a Grassman-like constant that exists between a given set of two corresponding partitions that exist among a given stringular encoder and its counterstring.