Part One of the Thirteenth Session of Couse 14

One-Dimensional superstrings of discrete energy permittivity differentiate kinematically over a sequential series of instantons, in so as to form two-dimensional world-sheets.  Two-Dimensional superstrings of discrete energy permittivity differentiate kinematically over a sequential series of instantons in so as to form three-dimensional world-sheets.  Two-Dimensional world-sheets form a traceable mapping that often works to take the hoop-like morphology that is of the non-time-oriented integration of indices that work to form the eluded to field at one distribution -- during one given arbitrary iteration of such a field during group instanton, while then taking the ghost anomaly that is formed by the directly related physical memory of the corresponding superstring, and integrating the eluded to multiplicit index of the tracing of the said given arbitrary superstring that is being discussed here through a Lagrangian -- into a cylindrical morphology, over time.  Two-Dimensional world-sheets often also form a traceable mapping that works to take the initial disc-like morphology of its initial non-time-orientable mapping, and integrates this mapping -- through a Lagrangian -- into shaft-like structures that twist in as static-based manner over time. Cylindrical-like world sheets of  two-dimensional world-sheets that directly correspond to one-dimensional superstrings, over a relatively transient period of time, twist over a sequential series of iterations when these bear a Doubolt-based format of traceable cohomological mapping.  World-Sheets that directly correspond to both one and two-dimensional superstrings often twist over a time-wise metric-based duration, in accordance with the directly related changes in directoralizations of the corresponding one and two-dimensional superstrings of discrete energy permittivity  This happens, in so that these may kinematically differentiate in their correlative world-tubes.  The three-dimensional world-sheets that exist are formed by two-dimensional superstrings.  I almost forgot to mention to you:  The world-sheet of a superstring involves not only the topological-based trajectory that is of the said superstring, yet, these also involve the direct field of the string that is Gliossi to the stringular neighborhood that is at the Poincaire level of any given said superstring.  These three-dimensional world-sheets tend to be torroidal in their basic shape.  I will continue with the suspense later!  Sincerely, Samuel David Roach.