Part One of Session Eight Of Course Five

What I am about to discuss is the general idea of the basis of light for when time is going through a tori-sector-range when the associated time that is related to such a Basis is only going forward.
There are operands in-between the point particles in the Ultimon at the moment when the Bases of Light are in their associated sub-Laplacian conditions, which is before the period in which such Bases are retied into the countless Planck Phenomenon related phenomena that comprise discrete units of energy impedance. Point particle density is where the condensed oscillations of the point particles exist. Strings form where the point particles become caught up in one another. Strings form as either vibrating strands or as vibrating hoops -- the latter of which are comprised of sundry strands that interconnect in a hermitian manner so that these approximate the hoops of which these behave like. When the related "Chis" concurantly bear "U"s that bear a relatively abelian concavity, these will allow for exclusively forward time moving superstings and Planck Phenomena related phenomena. When the "Chi" of certain of the Bases of light forms "U"s of opposite concavity than that of those that represent the basis of forward time momentum, this means that light is moving equally forward and backward in certain of the tori-sector-ranges that are operationally related to the affiliated Bases of Light during the course of the ensuing instanton that occurs over the course of the next iteration of Real Reimmanian Time. In certain parallel universe within the described tori-sector-range, time may here be exclusively moving forward or backward, yet, in the whole tori-sector-range as a unit in that section of the Ultimon, time would be moving equally forward and backward.
There is always some time moving forward in a tori-sector-range.
Time moving forward and backward required a Laplacian-based and hermitian non-abelian concavity in terms of a given Basis of Light just before the "push" that brings together instanton, since the limits of the "Chi" diagonals need to bear a smooth topology that is holonomically Real Reimmanian.
Aren't these posts more fun than a full-length motion picture -- if you can see what I am describing!
I will continue with the suspense later! Sincerely, Sam.