Gliosis-Sherk-Olive Fields Of Different Universal Settings

Let us here initially consider one given arbitrary GSO ghost of an orbifold eigenset -- that is of a Calabi-Yau manifold of a set of bosonic mass-bearing superstrings of discrete energy permittivity.  Let us next consider the Laplacian-based condition of such a cohomological mappable tracing -- as it is existing as a ghost-based pattern of the physical memory of a respective given arbitrary orbifold eigenset, that is of a Majorana-Weyl-Invariant-based mass, that is undergoing a tense of conformal invariance, over a sequential series of iterations of group-related instantons.  Let us say that the universal setting of the initially so-stated mass-bearing Calabi-Yau cohomological stratum, is of our respective universe -- as a set of superstrings that operate in so as to perform one specific function, in a state of what may be considered here as a tense of static equilibrium.  As an aside, the holonomic substrate of the topological setting of a bosonic superstring of discrete energy permittivity, is as a vibrating or oscillating hoop of space-bearing disturbance.  The so-stated bosonic-superstring-based orbifold eigenset of this case would have here been brought into a relative tense of conformal invariance by a group-attractor, that would have then acted in a tense of a Wess-Zumion interaction, in so as to form that correlative harmonic perturbation that would have worked to cause the relative optimum relaxation of the Gliosis-based topological stratum of the holonomic substrate of the so-eluded-to set of two dimensional superstrings, in so as to bring it into a relatively static tense of delineatory index -- at a proximal localized setting at the Poincare level of its Yukawa-based Hamiltonian operation.  Let us then say that the field-density of the GSO ghost-based indices that would work here to form the physical memory of the here discussed set of closed-loop bosonic phenomenology, would be, in and of itself, of a set of disc-like abelian differential geometry.  Let us then say that there would then be the Laplacian condition of the existence of a relatively countless set of bosonic superstrings, that would be in the same general state of condition as the so-stated orbifold eigenset of such a case -- yet of countless respective different universal settings -- that are inter-woven into the general proximal locus of what may be thought of here as the "annulus" of the field-density of the initially stated bosonic-related orbifold eigenset. This would then work to make the "appearance" of the field-density of the GSO cohomological setting of each of such orbifold eigensets, to seem as of more of a torroidal-based nature than otherwise. To Be Continued!  Samuel David Roach.