When one is to only vary in this general case, the gravitational force that is to here be Yukawa to the topological substrate of any one respective given arbitrary orbifold eigenset, over a set constraint of time -- the higher that the gravitational force is, that is Gliosis to the Ward-Caucy-based bounds of any one set orbifold eigenset, -- the more dense that the externalized shell of the said eigenset will tend to be, that is Gliosis to the immediate exterior of the so-stated orbifold eigenset, over the said set time constraint, that is to here be of one set gauged-metric that is to here be directly affiliated to what is to here be a relatively transient sequential series of group-related instantons. So, when only the increase that is of the respective given arbitrary gravitational force is to here be considered -- in the case of the relative density of one respective orbifold eigenset over time -- the case will tend to be to where, the higher that the Hodge-Index is, as to both the number of Schwinger-Indices that are to here be initiated from within the Ward-Caucy-based bounds of the holonomic substrate of the directly corresponding orbifold eigenset -- as well as when such a discrete increase in the number of the so-eluded-to gravity-based waves is to here be coupled with an increase in the net overall resultant scalar amplitude of the intensity of such integrative so-stated Schwinger-Indices, when this net increase is to here be in terms of both the cross between the correlative Hamiltonian pulsation of the said gravity waves & the extent of the topological sway that is of that wave modulae that is demonstrative of those Schwinger-Indices that act here as gravity waves, -- then, the higher that the density of the directly corresponding externalized shell that is to here be Gliosis to the immediate outer region of that core-field-density that is of the GSO cohomological topological stratum of the immediate exterioralized field of the so-stated orbifold eigenset is to tend to be, -- over the time-based constraint that is of the group-related metric by which the said orbifold eigenset is to be translated as a Hamiltonian operator, that is to be brought through its directly correlative Lagrangian-bases path, as it is being moved through its correlative Hamiltonian operand, via the directly related Fourier Transformation in which the so-eluded-to superstrings that act in so as to perform one specific function, are to be working together as one metrical-gauge-based operational-based index, is then to be as such.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
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