Session 10 Of Course 4

So, the local organization of the stuff that makes up a material thing is ordered differently, depending on if you are detecting that object as a globally distinguishable or as a substringular phenomenon.  Here.  Think of an electron.  It is the simplest point mass that always has a charge.  It has mass, it is in part kinetic energy, and the release of its spare energy when this energy is the result of the spin-orbital mode and angular momentum mode, of itself, is light.  We explained earlier what this J is, and why it is a mode.  When we as people detect an electron, it is basically a sphere of discharge that is altogether in a density of magnetism and charge.  This is a thing that appears as an individual entity that has components that are all near each other.  The quarks and leptons that make this up appear as individual things that are altogether and whose individual parts in the substringular are all near each other.  The strings of an individual quark of lepton are all next to each other in basically a majorized line that defines a small “eigenstate” of strings (taken as members of this “eigenstate.”)  Yet, the electron is not altogether in the substringular. (Although, these are completely in the substringular).  The quarks and leptons that comprise the electron are separated on different parts of what I term of as a tori-sector-range.  The field of the strings here (and not of their series iteration) of the electron form the whole eigenstate of such a tori-sector-range.  (A candy (doughnut) shape that’s like a real fat ring with a skinny holomorphic center.)  The field of the series iteration of a superstring may form a reverse-fractored eigenstate of a tori-sector-range.  The series iteration of the electron acts as the resultant of the activity of the energy of the strings that make the electron given as a whole basically parabolic.  In the substringular, the torus is a set of sectors of a tori-sector-range that work to describe the same electron.  I will explain better what a tori-sector-range is in course six.  Here, these ranges are not necessarily near, yet their Lorentz-Four-Contractions are so symmetrically geared that these appear near in the globally distinguishable.  One sector-range of a tori-sector-range may contain many subatomic pieces to many electrons.  I will continue with the suspense later!  Sam.