Some Knowledge As To Substringular Fields, A Special Case, Part One

Would you like an explanation of the phenomena of superstrings of discrete energy permittivity that act like a cross between one and two dimensional superstrings -- when in the globally distinguishable?  Well, here is an explanation.:  In order to begin explaining, I must write about certain occurrences in the substringular -- and then relate this to the globally distinguishable.  Picture a case bearing one of the simplest homotopic covariant-based modes:  Five inter-relating substrings are to here be considered in this case.  Three of these so-stated substrings are of a two-dimensional tense, while, two of these so-stated substrings are of a one-dimensional tense.  Let us now imagine the so-stated two-dimensional superstrings of discrete energy permittivity that are here being discussed, as closed strings that act as vibrating hoops that act in the transition kernel of the iteration of those first-ordered point particles that physically differentiate in nodal-lines that work to approximate a circular phenomenon, and, also imagine the so-stated one-dimensional superstrings of discrete energy permittivity that are being discussed here as open strings that act as vibrating strands that act in the transition kernel of the iteration of those first-ordered point particles that physically differentiate in nodal-lines that work to approximate a linear phenomenon.  The just eluded-to core-field-density of the said closed looped superstrings will form as an extraplolation that may be mapped-out as a toroidal-based phenomenon, while, the just eluded-to core-field-density of the said open strand-based superstrings will work to approximate a cylinderical-based phenomenon.  Let us now imagine that the two eluded-to open strings will, over time, work to make a best field-oriented fit in-between the so-stated two-dimensional superstrings.  The partial of these one dimensional superstrings would bear a fairly flush line of point particles that basically work to approach a line of first-ordered point particles that are acted upon by the natural curvature of space-and-time at the Poincaire level -- with the exception of any potential swivel-shaped bearing -- at a relatively minimum distance apart per first-ordered point particle that works to comprise the so-stated superstrings of discrete energy permittiivity.  These superstrings, too, approximate a neighborhood, after each reiteration that these are brought into BRST during each successive group-related instanton -- approximating a circular-based field -- in terms of the Majorana-Weyl invariant partial of one-dimensional superstings that orbit a given arbitrary conicentral-point, and, in terms of the Gliossi-based core-field-density of the said two-dimensional superstrings that work as the other general partial -- that works to comprise the eluded-to overall field.  Now, since all five of the given arbitrary superstrings of discrete energy permittivity -- that here work to bear a high degree of conformal invariance, are comprised by the pointal sequences that these superstrings work to determine, this is then here of a convergent eigenbasis.  The pointal sequences of these superstring here will then work to form a covariance, over time, that is also of a convergent eigenbasis.  Now, the series reiteration of the wave-pointal propagation has a relatively limited Real Reimmanian aptitude -- which I will elaborate upon later with this suspense!  To Be Continued!  Sincerely, Sam Roach.