Monday, December 15, 2014

Part Three of the Sixth Session of Course 18

Chiral cohomologies tend to depict harmonic topological-based flows of the mappable-tracing of the physical memories as to the where, how, and when, of any given arbitrary respective substringular kinematic activity.  This is while, antichiral cohomologieis tend to depict annharmonic topological-based flows of the mappable tracing of the physical memories as to the where, how, and when, of any given arbitrary respective substringular kinematic activity.  The kinematic activity of space-time-based fabric -- when in terms of both the existence and the activity of worm-holes -- tends to be a chiral-based spatial transposition, that is kinematically differentiable in both a harmonic and in an annharmonic manner, as one works to map-out the directly corresponding bending of space-time-fabric that is eminent to the multiplicit and multidirectoral-based Lagrangian-based nature of any one unique respective given arbitrary worm-hole, over time.  The harmonic differentiability of any one given arbitrary so-eluded-to worm-hole, is the even transfer of phenomena -- that enters in at one end of the so-stated worm-hole, while, such a respective so-eluded-to general format of physical phenomena leaves the other end of the so-stated worm-hole, relatively shortly after it does the so-stated initially mentioned entering of the worm-hole.  This is since the vast majority of the kinematic inter-play of the "speed" of any given arbitrary worm-hole is due to the contoursioning of space-time-fabric.  Yet, tachyonic transfer of phenomena happens a lot more often than many people may think.  If a phenomena of mass works to temporarily convert its light-cone-gauge topology from an abelian or Kaluza-Klein topology to a non-abelian or Yang-Mills topology, then, it is possible for the so-stated respective given arbitrary mass to temporarily become tachyonic.  A mass is typified as bearing of both a Kaluza-Klein light-cone-gauge topology, and also as bearing Yau-Exact singularities in-between its constituent superstrings.  So, a mass may be temporarily transferred as tachyonic at times -- simply by temporarily altering its light-cone-gauge topology.  The annharmonic nature of any respective given arbitrary worm-hole is contingent to the condition, that, the phenomena that leaves the said worm-hole at the exiting side of the so-stated worm-hole, tends to not be brought back to its potentially tachyonic origin.
This is enough for now!!! To Be Continued!  Sam.

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