Part Six Of Session 12 Of Course 19 -- The Klein Bottle And Orbifold Differentiation

Any given arbitrary worm-hole works to bear a Laplacian-based Grassman Constant -- that is both of a Njenhuis and of an unorientable nature.  The Laplacian-based condition -- that the Grassman Constant of a worm-hole is of a Njenhuis nature, is due to the physical quality that a worm-hole is the equivalent of the annulus of a bending and of a warping, of what was an initially Real Reimmanian space. The Laplacian-based condition -- that the Grassman Constant of a worm-hole is of an unorientable nature, is due to the physical quality, that a worm-hole is of the same general genus of space-time-based fabric as substringular phenomenology that is of a tachyonic-based nature.  This is true, even though a vast majority of the added velocity that any respctive worm-hole works to bring to any physical entity that is to be accelerated to go "faster than light," actually tends to be due to what is here to be just due to the so-stated condition of the fact that a worm-hole is a contorsioning or in other words of a bending of space-time-fabric -- that works to pull space-time-fabric into a further scalar locality of space, even if the actual speed that an entity itself that is pulled through such a said worm-hole, is not even moving close to light speed.  A worm-hole's speed actually tends to be basically due to the condition that the directly appertaining space-time-fabric that is of the said worm-hole -- is what is moving "faster than light," and not the respective holonomic substrate that is transported through it to be being transported "faster than light."  Yet, unorientable superstrings do always tend to become spontaneously tachyonic -- once these work to neither bear an orientable Grassman Constant during both the directly corresponding Beti Action and the directly corresponding Regge Action.  This is due to the condition that such a so-stated unorientable superstring is to here be temporarily altered -- from working to bear an initially  Kaluza-Klein light-cone-gauge topology into then working to bear instead a Yang-Mills light-cone-gauge topology.  This is due to the condition that a mass that works to bear a Kaluza-Klein topology, would need to bear an infinite fractal modulus in order for it to actually go at the speed or light or faster -- to where it would then need to bear all of the mass of the Continuum.  Yet, if one were to cause the so-eluded-to and temporary alteration of the light-cone-gauge of a mass-bearing superstring of discrete energy permittivity -- to alter into then work to bearing instead a Yang-Mills or in other words a non abelien light-cone-gauge topology, then, such a mass-bearing phenomenology can indeed go at the speed of light or faster.  Such an alteration of the correlative light-cone-gauge topology, is what will always tend to occur -- when the directly corresponding superstring is unorientable during both its directly corresponding Beti Action and its correlative Regge Action.  This is when a superstring will actually become tachyonic. I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.