More As To Calabi-Yau Manifolds And Worm-Holes

Just as a Calabi-Yau manifold has exited from a given respective arbitrary worm-hole, it (the respective Calabi-Yau manifold) will go back from working to bear a Yang-Mills light-cone-gauge topology, to working to then bear a Kaluza-Klein light-cone-gauge topology -- once again.  As the light-cone-gauge topology of the mass-bearing orbifold eigenset of this case returns from working to bear a non-abelian light-cone-gauge topology to then working once again to bear an abelian light-cone-gauge topology, -- the dimensional parameterization of the spatial-based Ward-Caucy bounds of the core-field-density, that is Gliosis to the so-eluded-to orbifold eigenset at the Poincare level, will then work to compactify from that added dimensionality-based condition that it had had in the worm-hole that it had just exited, -- to then simply bearing those initial d-fields (for electrons) and f-fields (for nucleons) that the directly corresponding Calabi-Yau manifold of that respective tense of an orbifold eigenset that had here just traveled thru a worm-hole, was to initially work to bear, as a Noether-based tense of a set of substringular eigenindices that are to tend to be Yau-Exact, for all intensive purposes -- once the said orbifold eigenset has finished bending through space amongst the immediately prior venue of those critical cusps that had eluded-to the process that is here of the transfer of physical phenomenology, along a contorsioning delineatory-based Lagrangian displacement, that is of that Hamiltonian operand that had here acted as the previous translated worm-hole eigensbase.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.