Session 15 Of Course Nine

The light-cone-gauge multiplicitly exists between Planck phenomena and superstrings.  The light-cone-gauge corresponding to one-dimensional superstrings consists of five mini-string segments that are in-between an arbitrarily corelative Planck-like phenomena ansd its corresponding one-dimensional fermionic string.  With a bosonic string, there are ten mini-string segments in-between the corelative Planck phenomena and its two-dimensional bosonic superstring.  When a one-dimensional superstring closes via the Fujikawa Coupling as may be mathematically described when using the Greene function, the five doubled up milni-string segments unravel and reconnect to form ten mini-string segments that connect homogeneously along the newly formed two-dimensional bosonic string.  So, when a two-dimensional bosonic superstring undergoes such a Yakawa Coupling via the Greene function to open to form a one-dimensional fermionic string, the ten mini-string segments mentionesd double-up to form five mini-string segments after the ten mini-string segments that were previously mentioned are released and ravled to reconnect in a homogeneous manner.  These switches in mini-string happen during iteration or instanton with the help of gauge bosons.  Gauge bosons are an example of two-dimensional superstrings that are larger than superstrings.  Gauge Bosons spin and roll to allign the light-cone-gauge during the activity that occurs during BRST.  BRST is when the Imaginary exchange of Real residue happens among superstrings that are discrete energy permittivity and their counterparts.  (The counterparts of such mentioned superstrings act as a substrate for the said strings.)  The gauge bosons act as "light-switches" that activate the other heterotic strings.  I will discuss what I mean by that in future courses.  As the gauge bosons counterspin and counter-roll, the corresponding activity levers thru space in a hyperbollic manner so that the other heterotic superstrings are able to spontaneously open when necessary so that their counterstrings may retie as one-dimensional superstrings during certain circumstances, and also so that other phenomena that is directly attached to the corelative substringular encoders may undergo the proper retying during the metric in-between instantons when such retying is prominent.