Chern-Simons Invariants And Orbifolds, Part One

An orbifold eigenset is a set of a discrete quanta of energy, that operate in so as to perform one specific function.  The individually taken discrete quanta of energy -- that work in so as to comprise any one of such so-mentioned orbifold eigensets -- act as being delineated along the outer surface area of the so-stated respective given arbitrary orbifold eigenset, that is of any one respective unique cases.  This is analogous to the physical condition, that if a point-related charge is in the center of a conductive shell -- all of that charge is here to be delineated at the outer surface of that shell.  Next -- let us consider a given arbitrary orbifold eigenset, that is here to bear both hermitian Lagrangian-related singularities and hermitian-related metrical singularities, -- over an evenly-gauged Hamiltonian eigenmetric.  This would then mean, that the said orbifold eigenset of such a respective case, is to be transferred in this case -- via a Rham (De Rham) cohomology, -- as it is here being conducted through a sequential series of group-related instantons, in the course of a correlative Fourier Transformation.  Let us next say that the said respective orbifold eigenset, is to consist of a relatively significantly large Hodge-Index of discrete energy quanta.  This means that there are here to be many individually taken discrete energy quanta that are here to work to comprise the respective orbifold eigenset -- that is of such a case.  The orbifold eigenset is to here to behave as one particular genus of field, over the directly corresponding relatively transient evenly-gauged Hamiltonian eigenmetric.  The said individually taken discrete quanta, that are here to work to comprise the respective orbifold eigenset, are here to be delineated in a spatial-related covariance -- per each individually taken group-related instanton, in such a manner -- to where the angular-canonical flow that may be extrapolated, when this is taken in comparison to the layer of proximal locus, that these said discrete energy quanta are here to work to bear, -- when these are here to be compared to each other in a Laplacian-related manner, per each individually taken iteration of group-related instanton, in which such an orbifold eigenset is to here to be undergoing the earlier mentioned evenly-gauged Hamiltonian eigenmetric, is here to work to gauge, to an extent -- where the correlative discrete quanta of energy that are here of the same universal setting, that are here to work to comprise  their integral-related individually taken parts of the same orbifold eigenset of such a case --are then to be placed at, per each succeeding iteration of group-related instanton.
I will continue with the suspense later!  To Be Continued!  Sincereley, Samuel David Roach.

Superstrings At Surface Area Of Shell

Those individually taken discrete quanta of energy, that work to comprise the topological stratum of any one given arbitrary orbifold eigenset -- tend to exist, during any one given arbitrary iteration of group-related instanton, at the general region that is proximal local to the surface area of the outer shell of the respective given arbitrary orbifold eigenset, that is of any one specific given arbitrary correlative case.
This is allegorical to the condition, that a charge that is to be formed at the center of a conductive shell -- will tend to be delineated at the outer surface area of that self-same shell.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Harmonics Of Vibrating Open Loops

When one is here to be considering a Ward-Cauchy-related open-loop phenomenology, that is isotropically stable -- such as a (1+1) string -- such a said superstring of discrete energy is to tend to harmonically vibrate mildly, during any given arbitrary iteration of BRST, in which it is here to then to work to form a tightly-knit homological eigenstate, at the proximal local region that is Poincare to the core-field-density of the topological stratum of the so-stated open-loop phenomenology.  Such a said (1+1) string, though, is to vibrate mildly in an anharmonic manner, during the directly corresponding sequential iterations of the generally unnoticed duration of Ultimon Flow.  Yet -- when one is here to be considering a Ward-Cauchy-related open-loop phenomenology, that is isotropically unstable -- such as a (2+1) string -- such a said superstring of discrete energy is to tend to vibrate mildly in an anharmonic manner during any given arbitrary iteration of BRST, in which it is here to then to work to form a tightly-knit homological eigenstate, at the proximal local region that is Poincare to the core-field-density of the topological stratum of the so-stated open-loop phenomenology.  Such a sad (2+1) string, though, is to vibrate mildly in a harmonic manner, during the directly corresponding sequential iterations of the generally unnoticed duration of Ultimon Flow.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.