Part One of the Thirteenth Session of Course Six

Well hello again world, this is Samuel Roach here!  I hope that you are having a phenomenal day!
Here is the first part of the thirteenth session of course six.
                
There is a space at the end of each Chi-related endpoint that extends beyond the central substringular encoder of each general world-sheet (that is, of each Main world-tube).  This space is interconnected to the general stratum of the substringular via mini-string.  This space is always just a fraction of a radii from the endpoints of the semicircles and the upside-down semicircles of a cross-sectional region of the Royal Arc where there is to be a Basis of Light to differentiate via a sub-metric that happens right before instanton-quaternionic-field-impulse.
This region here is due to the fields exerted by the substringular encoders of the world-sheets that are located here.  All superstrings have fields associated with them.  One dimensional stringular fields tend to be thinner than the fields of two-dimensional superstrings (with the exception of certain relatively large Gliossi-Sherk-Olive fields that relate to certain one-dimensional superstrings that are undergoing  a strong degree of regional conformal invariance).  The integration of all of the superstrings that indirectly associate with one of the semihooops supports the existence of the described semihoop.  The slight curve inward that the recycleable material has to travel through is why when stringular residue is first taken up, there is a slight "time" or gauge-metrical lag that happens,and this so-called "lag" allows for the observation of kinematic Fourier or the discernment of time-wise active differentiation.  Once this lag is brought to the point of the Royal Arc where the pointal material may be recycled promptly, the travel of phenomena in the general world-sheets responds to Ultimon speed just about instantaneously.  The only factor here now would be the recycling mode as I taught in lessons earlier, and as I will teach later.  Superstrings in the substringular may only be so close due to the fields that these exert.  The fields that superstrings exert generally repel when these fields oscillate asymetrically , especially when these mentioned strings are encoded for as coming from another general world-sheet.  This extra need to repel is due to the extremely different sequences of the strings between these AND also their differences in how the waves in these are built up at any given instant (series iteration differentials).                                                                                            
I will continue with the suspense later!  I hope for the best of all of my readers.
I think of mankind as my family.  I won't lose, because I have Tau on my side!  God Bless!  Sincerely, Sam.