Correlative Clifford Expansion And Orbifolds

Let us initially consider a relatively small set of adjacent orbifold eigensets -- of which are here to be, in part, comprised of discrete quanta of energy permittivity, that are to each (each combination of the individually taken superstrings and their immediately corresponding counterparts) work to bear their correlative Lorentz-Four-Contraction, as each of such individually taken combination of superstrings and their correlative counterstrings -- are to work to bear their correlative scalar amplitude of their directly corresponding Polyakov Action eigenstate -- as the so-stated adjacent orbifold eigensets of such a case scenario, are to bear the overall composition of those directly involved superstrings and counterstrings -- that are here to bear their hightened Clifford Expansion (as to the inverse of what their Lorentz-Four-Contractions would then bear) -- in accordance to their covariant velocity, when this is made in both a codeterminable and in a codifferentiable manner, relative to both the existence and the motion of electromagnetic energy.  Let us then say, that each of the individually taken superstrings of such a case -- may be said to be adjacent to each other -- when this is taken in an individually taken euclidean-based manner.  This would then mean, that the substringular situation of such a case -- is a given arbitrary example of a Minkowski-based flat-space region.  This would then, as well, mean that all of the said individually taken superstrings of such a case -- that are of the so-stated adjacent-based manner -- will then work to bear a euclidean tense of an orphoganal vibrational oscillation, when this is to be taken as any of the one of such individually taken superstrings of discrete energy permittivity, -- as to here be covariant in its explication upon any of the other of such so-stated given arbitrary individually taken superstrings of discrete energy permittivity, that are of this respective given arbitrary case scenario.  This would then, as well, -- mean, that the directoral-based topological sway of the sub-Fourier-based activity of the expanding Clifford-based interaction of the decompactifying superstring and its correlative decompactifying counterstring, -- is to bear a conformally invariant-based metric-gauge-based set of indices that are here to indicate the specific mannerisms of the inversely Lorentz-Four-Contracted individually taken superstrings -- that are here to be undergoing the Polyakov Action -- in so as to bear a well-suited set of Ward-Caucy-based conditions -- so that the overall angling of the directly corresponding superstrings that are to here be iterating as a set of moving discrete quanta of energy, that as well, work to bear a Majorana-Weyl-Invariant-Mode that is Poincare at the Noether-based region that is academic to the permutative Fourier-based field, by which the said orbifold eigensets are moving, yet not so much when this is taken into consideration amongst the other respective covariant superstrings of this said case -- is to still bear both the so-eluded-to codifferentiable and the so-eluded-to codeterminable genus of such a so-stated euclidean-based angling of the respective orphoganation, over the duration by which the so-eluded-to group-metric is to bear the so-eluded-to Fourier-differentiating Yukawa-based Noether field of such a respective given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Affiliated With Light-Cone-Gauge Expansion

Let us initially consider a given arbitrary discrete quantum of energy, during the course of one specific given arbitrary iteration of BRST.  Over the course of such a so-eluded-to duration -- both the directly corresponding superstring of discrete energy permittivity, and, its immediate superstringular counterpart -- are decompactified to the inverse of the extent that these are Lorentz-Four-Contracted.  This so-stated process of decompactification, may be called the Polyakov Action.  Due to the condition, that the correlative Fadeev-Popov-Trace eigenstate, that is to directly correspond to both the said superstring and its said counterpart -- does not work to decompactify with the so-eluded-to discrete quantum of energy permittivity, -- as both the so-stated superstring and its superstringular counterpart are in the process of being decompactified, there is a hyperbollic-based Clifford Expansion that is to here occur, in the Laplacian-based Hamiltonian-based region, that is to exist in-between the correlative superstring and its directly corresponding Fadeev-Popov-Trace eigenstate, over the course of the said iteration of BRST.  Any given arbitrary superstring, is to bear an oscillation during BRST -- that is to be both codeterminable and codifferentiable in a pseudo-based Fourier-related tense, as being of a of a euclidean tense of orphoganation -- with any adjacent respective given arbitrary superstrings, that are of the same universal-based setting in the substringular.  Adjacent superstrings that are of the same universe, may potentially vary completely in the extent by which their Lorentz-Four-Contractions are to bear as a Laplacian-based scalar amplitude by, and thus, by which their Polyakov Action eigenstates are to then bear as their individually taken scalar amplitude -- in the manner in which these do.  This will then tend to cause the correlative tense of the wobbling of the directly affiliated second-ordered light-cone-gauge eigenstates, as well as the correlative tense of the vibrational oscillations of both the respective superstring, its counterpart, and the correlative Fadeev-Popov-Trace eigenstate, -- to tend to bear such a tense of conformal invariance -- that will work to help suit both the directly associated Laplacian conditions and the directly corresponding Fourier-based conditions, in so as to bear the necessary tense of wobble, while still working to bear the necessary tense of the inverse activity of the so-stated Polyakov Action eigenstate, that may here be attributed to the correlative and the respective scalar amplitude of the here pertinent tense of its Lorentz-Four-Contraction, over the course of the said iteration of BRST of this respective given arbitrary case scenario. 

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Altered Field And Kahler Conditions

Let us consider an initial case of a superstring of discrete kinetic energy, that is to act here as part of the overall activity of a moving electron, that is in time and space -- to where the so-eluded-to discrete quantum of kinetic energy permittivity is to be moving here, in such a tense of holomorphicity, to where its core-field-density may here be extrapolated, as working to bear a washer-like cohomology, with a relatively small annulus set in a Laplacian-based manner, at its relative center.  Let us say that, at a specific arbitrary set locus in time -- the so-eluded-to one-dimensional superstring of discrete energy permittivity that works here to help to comprise the said electron, is to be caused to move, in such a manner, to where its field is polarized -- in the process of the said superstring to here be in the process of being propagated across a relatively mean Lagrangian-based path, over time.  This would then tend to cause the core-field-density of the so-stated respective superstring, to alter from bearing its initial so-stated washer-like cohomological field, to then subsequently bear, instead, a conical-like shaped cohomological field -- at the Poincare level that is Gliosis to the said superstring's core-field-density.  Such an alteration in the core-field-density of the so-stated one-dimensional string, would then tend to form Chern-Simons singularities -- in both the considerations of the potential spurs that would then often tend to thus happen to the metrical-based tracing of the said open-loop superstring, as well as in consideration of the potential spurs that would often tend to thus happen to the Lagrangian-based tracing of the same said open-loop superstring.  This potential formation of the so-eluded-to Chern-Simons based singularities, would then often tend to work to help in the consequential formation of a proximal localized antiholomorphic Kahler condition, which, would then tend to work to cause an ensuing eigenstate of the Kahler-Metric to then be initiated upon the said one-dimensional superstring of discrete kinetic energy of such a given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.