Part One of the Seventh Session of Course 16

Topology is the description of the surface of superstrings and/or the surface of Fadeev-Popov-Trace eigenstates and/or the surface of mini-stringular phenomena.  Superstrings are comprised of first-ordered point particles that come together to form either one dimensional phenomena that act as open strands or two-dimensional phenomena that act as closed loops.  First-Ordered-Point-Particles are individually comprised of a "ball" of mini-string that may be compared -- allagorically, to a "ball of yarn."  It is mini-string segments that work to form the holonomic substrate of the core field density of the substringular.  So, when one is to consider the "topography" of superstrings, and/or the "topography" of Fadeev-Popov-Trace eigenstates, and/or the "topography" of mini-string segments, and/or the "topography" of light-cone-gauge eigenstates, respectively, one is to then be considering here the "topographical" condition of the said given arbitrary topology of the just eluded to substringular phenomena.  Homotopy is the format of the conditionality of superstrings that appertains to the manner as to how the various substringular phenomena are interconnected as a whole in the multiverse by core field density eigenstates -- that act as mini-string segments that inter-bind in one manner or another, for all substringular phenomena that are unfrayed by the various activities of the given existent black-hole-like phenomenology that exist at any given arbitrary group metric that may here be considered.  A very important manner of considering as to what the genus of any given arbitrary topology that is to be considered at any given arbitrary instant under consideration is the genus of the directly corresponding light-cone-gauge eigenstate that would then here be correlative to whatever the so eluded to substringular scenario is being considered -- at the eluded to instant under consideration.  It is the general activity of the phenomenology of the light-cone-gauge that works to form both the template of those vibrations that work to activate the various Rarita Structure gauge-metrics, as well as to form the means of that "spring-like" activity that works to pull both superstrings of discrete energy permittivity and Fadeev-Popov-Trace eigenstates of discrete energy impedance into the generally unnoticed portion of Ultimon Flow -- in so that the eluded to substringular phenomena may be "primed" to move into their ensuing distribution-based delineations, in so that the sequential series of group instantons may move in the multiplicit genus of direction that it is encoded to go into.  There are two different formats of light-cone-gauge topology -- there is the non-abelian genus of a light-cone-gauge, that is known of as a Yang-Mills topology, and, there is the abelian genus of a light-cone-gauge, that is known of as a Kaluza-Klein topology.  In both respective topological formats of light-cone-gauge genus, there is that general genus of light-cone-gauge that appertains to the light-cone-gauge structural-basis for one-dimensional superstrings, and, there is that general genus of light-cone-gauge that appertains to the light-cone-gauge structural-basis for two-dimensional superstrings.  In different respective cases, there are one-dimensional superstrings that may be either of a Yang-Mills light-cone-gauge topology, or, of a Kaluza-Klein light-cone-gauge topology -- given what the scenario calls for, and, there are two-dimensional superstrings that may be either of a Yang-Mills light-cone-gauge topology, or, of a Kaluza-Klein light-cone-gauge topology -- given what the scenario calls for.  It is the combined conditionality as to what both the light-cone-gauge topology is, and the format of both the hermitian and/or the Chern-Simmons genus of a substringular setting, that works to help define as to whether any given phenomenon is of either a state of electromagnetic energy, a state of plain kinetic energy, a state of mass, a state of discrete units of entropy-based eigenstates, the general condition steady-state eigenstates that exist in worm-holes, or, the general condition of perturbative-based eigenstates that exist in  worm-holes.  I will then here end with these just stated general descriptions as to what the topological formats of the various conditions that appertain to light-cone-gauge eigenstates are -- until I commence with a further elaboration.  I will continue with the suspense later!  Sincerely, Samuel David Roach.