Let us here say that one were to have an orbifold eigenset, that was comprised in a Laplacian-based manner -- of a relatively flat overall topological surface, that is here constructed of an exterior "sheath" of fermionic superstrings of discrete energy permittivity -- that would here work to physically surround relatively few bosonic superstrings of discrete energy permitivity that are localized in a Majorana-Weyl-Invariant manner at the interior of the said orbifold eigenset. So, one is to here have a substringular tense of set of fermionic discrete quanta of energy, that works to surround -- in a Laplacian-based manner under the correlative Ward-Neumman physical boundary conditions -- a relatively small set of bosonic superstrings of discrete energy permittivity. As the so-eluded-to orbifold eigenset of such a case, is to move in a given number of spatial dimensions plus time (let's say that the said orbifold eigenset of such a given arbitrary case were to be moving in 12 spatial dimensions plus time), -- in such a manner in so as to be moving flush in the respective relative forward-holomorphic direction over time -- there will be a correlative Laplacian-based coniaxial that may be considered here, to allow for an 11 dimensional parametric coniaxion that may be plotted here as a physical extrapolation, that would then allow for the involvement of the so-stated orbifold eigenset to bear a respective topological sway, that would consequently ebb back-and-forth in a piecewise continuous manner in all 11 of the so-stated dimensional-based parametric coniaxials, over a sequential series of instantons. In the process -- the world-sheet-based cohomology of such a given case, if it is here of an efficient manner, will work to bear a conical external-based core-field-density at the Poincare level of the external surface of the Gliosis-based field, that is tangent to the topology of the said cohomology -- that will here work to bear its relatively hermitian tip of singularity at its apex, to angling in the direction of the mean Lagrangian-based path that is supplemental to the average directoral topological sway that is directed against it as a resultant that is Yukawa in all 11 of such said coniaxials over time. Two of such coniaxials will here be of a Real Reimmanian nature, and 9 of such coniaxials will here be of a Njenhuis nature. The metric that is here involved with the Slater-based state --- that works to describe this process of the said orbifold eigenset, as moving in a best hermitian fit in the multidimensional mean Lagrangian path that is along the correlative Hamiltonian operand of such a Hamiltonian operator -- will be of such a gauge-metric pulsation in a piecewise continuous manner -- that will end up acting in so as to bear its genus of metrical singularities that are formed, by what the incoming external forces that are to act upon the said orbifold eigenset are to be delineated as.
I will continue with the suspense later! To Be Continued! Sincerely, Sam Roach.
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