Part Four of the Sixth Session of Course 18

Phenomena that is contingent to that of a mass that enters a worm-hole is of a bosonic nature, so that the phenomena that is propagated through the said worm-hole works to obey a tense of the correlative Lortentz-Four-Contractions that work to effect it, over the group metric in which the so-stated phenomena that enters the said worm-hole -- in a manner in so that the initially eluded-to mass is transferred in here as having a Yang-Mills light-cone-gauge topology, in a tachyonic manner, through the multiplicit and multidirectoral curl-based curvature of space-time-fabric. That scattering of the so-eluded-to mass that is made tachyonic, by the altering of its light-cone-gauge topology -- is a perturbation of the directly related given arbitrary Calabi-Yau action.  The kinematic activity of such a perturbation in the Calabi-Yau action is a perturbation of the correlative given arbitrary Calabi-Yau metric.  And, the so-eluded-to phenomenology that is perturbated out of the tendency of that mass from having the initial Kaluza-Klein topology -- to having, instead, a Yang-Mills topology (in order to here be of a tachyonic nature), is a perturbation of a given arbitrary tense of a Calabi-Yau manifold. The projection of such a perturbated manifold of an orbifold eigenset of a mass is a respective given arbitrary example of a perturbative Calabi-Yau projection.  The cohomological-based nature of such a Rayleigh-based scattering, is a genus of a perturbative Gliossi-Sherk-Olive projection, since this respective given arbitrary tense of an annharmonic scattering is an alteration in the mode of an initial tense of one unique respective given arbitrary unit of a discrete mass, in this case.  Yet, since the propagated cohomology of a mass in and of itself -- in terms of the hermitian nature of its Poincaire-based indices --  that is transferred through a worm-hole, tends to be  harmonically delineated, in the course of its propagation through the said worm-hole, it works to bear a harmonic and thus a chiral cohomological symmetry that is either of a trivially isometric or of a non trivially isometric geometric correlation.  Yet, if the delineation of a phenomenon that is propagated through a Lagrangian works to bear an assymetric cohomological genus, that is thus an antichiral cohomology, over time, then, its said cohomology may be termed of as a Kosoma-Suzuki cohomological index.  The scattering of light -- in and of itself, forms a cohomological-based patterning, that is an example of a Kosoma-Suzuki cohomology (since it is of an assymetrical-based nature, that is thus, an antichiral cohomology).  Both symmetric and assymetric cohomological-based projections are examples of Gepner models.  The potential energy of a superstring may be termed of as a superpotential.  Such a potential may be considered here in terms of what is known of as a Landau-Gisner potential .
To Be Continued!  Sam.