Part Two To the Twelth Session of Course 13

Partitions of one-dimensional superstrings of discrete energy permittivity go from just to the Njenhuis right of the general topological mapping of the said format of string to just to the Njenhuis left of the same general topological mapping of the same format of string -- from  the reverse-norm-to-holomorphic end of the said superstring to the forward-norm-to-holomorphic end of the same said superstring..  For two-dimensional superstrings of discrete energy permittivity, the said partitions go from being off of the general topological mapping by being both just to the forward-holomorphic direction and also just to the Njenhuis right of the directly related topological mapping at the same metrical duration To being off of the general mapping by being both just to the reverse-holomorphic direction and also just to the Njenhuis left of the directly related topological mapping at the same metrical duration -- from the forward-norm-to-holomorphic end of the superstring counterclockwise to up to all around the general topological mapping of the said string.  The format of point particles that work to comprise the topology of superstrings most directly are first-ordered point particles -- as I have described in prior posts.  The fabric that works to comprise first-ordered point particles is a holonomic substrate that is comprised of a "yarning" of substringular field -- a yarning of what I term of as mini-string segments.  Such mini-string is a composite of second-ordered point particles that are beaded together in so as to have a cross-sectional thickness of 10^(-129) of one meter thick in the substringular.  Again, the diameter of a first-ordered point particle in the substringular is 10^(-86) in the substringular.  So, even though most phenomena tends to be radially dependent, point particles are dependent more on a basis of their diameter.  The counterstrings of superstrings -- that are here of discrete energy permittivity --  have partitions that are reverse delineated when relative to their directly related superstrings.  The partitions of one-dimensional counterstrings  that are of discrete energy permittivity go from just to the Njenhuis left to just to the Njenhuis right of the topological stratum of the said counterstring -- from the reverse-norm-to-holomorphic end to the forward-norm-to-holomorphic end of the said one-dimensional superstring of discrete energy permittivity.  For the partitions of two-dimensional counterstrings that are of discrete energy permittivity, the format of the directly related partitions goes from both just to the Njenhuis left and to just to the reverse-norm-to-holomorphic side of the general mapping of the topology of the corresponding string to being both just to the Njenhuis right and just to the norm-to-forward-holomorphic side of the general mapping of the topology of the corresponding superstring.  Again, just as with the superstrings that are directly related to the just mentioned counterstrings, the partitions may often be delineated from the norm-to-forward-holomorphic end of the said counterstring all of the way around its topological stratum in the counterclockwise direction of assorted Laplacian-based distribution(s).  I will continue with the third part of this session later!  To Be Continued!  Sincerely, Sam Roach.