What Charge Is

The following is a reductional view,  as to what physical electrodynamic charge is:

Electrodynamic Charge Is The General Action Of Chern-Simons Invariant Perturbation, as Taken
Along The Topological Stratum Of A Mass-Bearing set of cohesive discrete energy, -- in which such a set of cohesive discrete energy, is here to be operating to perform a common function. Sam Roach.

A Balance, Working To Help Form Steady-State

When an orbifold eigenset is to be undergoing a tense of superconformal invariance, there will tend to be a proximal local balance, --  between the kinematic activity of the Poisson-related functioning of such an eigenset, And, the kinematic activity of the Green-related functioning of such an eigenset, that is here to be most associated with the covariant flow of the delineation of those discrete quanta of energy, that are here to work to comprise such an inferred set of discrete quanta of energy, that operate to perform one specific task -- to where such a "team" of discrete energy, that are here to work to make-up this holonomic substrate, will consequently tend to be of a mass-bearing topological-related stratum. This is a reverse-fractal, of what one would normally think of as being of a steady-state scenario.  Samuel Roach.

Eminent Knotting Along The Rarita Structure

Any given arbitrary eigenindex of the Majorana-Weyl-Invariant-Mode, is formed by the resultant interaction, of a general genus of an eminent Ward-Cauchy-related knotting in the realm of the substringular, -- as this is here to be considered, when taken to be existent along the general topological stratum of the Rarita Structure. I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Substringular Motion And The Morphology Of Space-Time-Fabric

Whenever a substringular phenomenon is to move, over the course of time, -- it will tend to make at least some sort of an effect, upon part of the morphology of the topological stratum of space-time-fabric.  I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

The Flow Of Cohomology & The Motion Of Discrete Energy

The Gliosis-based interaction of point commutators, with the topological stratum of discrete energy quanta -- when this is as taken at the Poincare level -- works to help form, what may be termed of here as being cohomology.  The attraction/repulsion-related characteristics, of the multifarious sets of the ordered groupings of cohomological eigenstates (cohomological eigensets), helps, in the process of working to drive discrete energy into motion -- so that discrete energy may be able to move, so that it may be able to both persist and exist.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Annharmonically Scattered Orbifold Eigenset

Let us initially consider an orbifold eigenset, that is undergoing a Majorana-Weyl-Invariant-Mode.  It is thus, at the moment here, under the Ward-Cauchy constraints of a tense of conformal invariance, or, in this case, of a tense of superconformal invariance -- at an internal reference-frame, that is Poincare to the topological stratum of the said orbifold eigenset. Such a superconformally invariant orbifold eigenset, is here to tend to be exhibiting a De Rham cohomology.  It is then to be scattered, via a Rayleigh scattering, of which is of an annharmonic scattering.  This will then tend to mean, that the orbifold eigenset that is of such a case -- will tend to be perturbated out of its initially stated De Rham cohomology, into a Doubolt cohomology, at least initially -- in the process of being scattered  out of such a tense of a Majorana-Weyl-Invariant-Mode.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gravity And Warped Light-Cone-Gauge Eigenstates

High amounts of gravitational force, will often act in so as to work at warping the topological stratum of those light-cone-gauge eigenstates -- that are proximal local to such a high application of gravitational force.  Whereas -- high amounts of anti gravitational force, will often act in so as to work to reverse such an earlier mentioned warping of the topological stratum of light-cone-gauge eigenstates -- that are proximal local to such a high application of the said anti gravitational force.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Next Part Of Partition-Based Discrepancies

The expression i*PI(del) -- refers to the holonomic substrate of the homotopic residue that is gained and/or lost, as the partitional-based discrepancies (as a topological stratum) -- that are indirectly utilized, are here to help at the generation and/or the degeneration of homotopic cohomological phenomenology -- for one orbifold eigenset per instanton, as may be averaged over an evenly-gauged Hamiltonian eigenmetric over time.  With any unscattered electromagnetic energy, there is to be no net gain nor loss of such so-eluded-to increments -- to where there is here to be no net gain nor loss of partition-related discrepancies per each individually taken orbifold eigensets of such electromagnetic energy, over the course of any one set instanton in which such an electromagnetic tense of phenomenology is here to be unscattered.  (This is to where the said electromagnetic energy is here to neither strike the externalized core-field-density of any light-cone-gauge eigenstate, nor, even more potentially rarer, no electromagnetic energy that is here of the earlier mentioned nature is to strike head-on.)
I will continue with the suspense later!  To Be Continued!  Sincerely, 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.

Mini-Stringular Segmentation And First-Ordered Point Particles

Mini-Stringular segmentation is drawn into nodes -- in a multiplicit manner, in so as to work to form what may be termed of here as being the essence of first-ordered point particles.  First-Ordered point particles come together as building blocks of the topological stratum of discrete energy permittivity, in so as to work at helping to form both superstrings of discrete energy permittivity, as well as these said superstrings' counter parts.  First-Ordered point particles are also existent, in so as to work to help at forming part of the topological stratum of norm-state-projections.  These node-like holonomic substrate-based phenomenology, of what I have just termed of here as being first-ordered point particles, come in the form of a parabolic-shaped twining of mini-stringular segmentation, -- of which is utilized, in so as to work at forming that level of Ward-Cauchy-related building blocks, -- that exist multiplicitly at one level of the holonomic substrate of topological stratum that is below the composition of discrete energy itself.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Relative Pulse Of Norm-State-Projections

Since a Hausendorf norm-state-projection of one given arbitrary length, as this is taken along its topological surface at the Poincare level, will tend to work to bear a higher Hodge-Index than a Campbell norm-state-projection that is of the same given arbitrary length, as this is taken along its topological surface at the Poincare level --as this is correlative to the number of first-order point particles that work to comprise the correlative phenomenology of both such a  said comparative Hausendorf projection when in relationship to a said Campbell norm-state-projection, when this is taken in terms of the  holonomic substrate of the topological stratum of the said Hausendorf state in comparison to the latter mentioned genus of projection, when only working to consider this factor alone, such a respective given arbitrary Hausendorf norm-state-projection will then tend to bear a higher Hamiltonian-based pulse than a correlative Campbell norm-state-projection.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Characteristics For Topological Extrapolation

There are a few general categories of topological extrapolation, that I can think of from scratch -- that may work here to bear a given arbitrary extrapolation, in so as to further to be able to understand even better, the respective correlative holonomic substrate of topological stratum -- that is to here to be directly associated with certain given arbitrary Ward-Cauchy-based phenomenology, that is here of a substringular nature, over time.  1)  Consider both the Laplacian-based nature as well as the Fourier-based nature, that is of both that spatial and that dimensional compactification-based tense, -- by which any respective  orbifold eigenset, is then to be able to be extrapolated as one holistic entity.
2)  Next, -- consider the nature of both the fractal and the elastic module, if you will, of the topological stratum, that is Poincare to the Gliosis-based surface, of the here respective orbifold eigenset.
3)  Furthermore, -- consider both the Laplacian-based Ward-Cauchy conditions and the Fourier-based Ward-Cauchy conditions, by which the correlative knotting that is to be taking place here, from within the physical bounds of the said respective orbifold eigenset, is to happen, --  as both a time-related phenomenology and also as a non-time-oriented metric-gauge-based holistic quantum of energy, that is to be pulled into its kinematic group-related activities, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Mini-Stringular Segmentation And Substringular Fields

Mini-stringular segmentation is built-up of second-order point particles -- that are "chained" or linked together, in a chord-like manner.  It is mini-stringular segmentation, that works to act as that holonomic substrate -- that functions as that general genus of topological stratum, by which substringular fields are thus to be formed.  For instance -- it is the multiplicit strands of phenomenology, that are at least partially comprised of by the said general genus of mini-stringular segmentation -- that work, in so as to allow for those field-based interactions among superstrings, to then to be able to happen.  Furthermore -- it is the multiplicit mini-stringular segmentation, that acts in so as to both directly and to indirectly interconnect the quantum world of discrete energy together, into the general condition of homotopy, -- over the course of each succeeding iteration of group-related instanton.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Briefly As To Why Energy Is Particle And Wave-Like

Mass is energy in static equilibrium.  Energy is motion.  Motion is a set of one or more corelating disturbances in space.  So -- what makes such motion as both a particle-like and as a wave-like phenomenology, in so as to be a multiplicit holonomic substrate of topological stratum?
It is the metric-gauge-related pulsation, that is of the covariant eigenindices of the multiplicit disturbance of space, that work to become of such a manner that is both codifferentiable and codeterminable as interdependent eigenstates that exist in space -- that acts as the generic "force," if you will -- that acts in a Fourier-based manner, in so as to work to form that grand unification of field that is to exist, in order for energy to both exist and persist as a set of particles that act as waves, in the arena of space-time-fabric, so that any superstrings of discrete energy permittivity may be able to exist at all -- in their respective Calabi-based manifolds, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Light Intensity And Orbifold Abrasion

The higher that the intensity of electromagnetic energy is, upon the proximal locus of the topological stratum of a given arbitrary orbifold eigenset, over a set group-metric of time, -- the more that there will be the potential tendency of there then being a higher density of infrared photons, that are to likely be at the said proximal locus of the topological stratum of the respective given arbitrary orbifold eigenset, over that same said group-related metric.  As said before, the higher that the intensity is, of infrared photons upon the proximal locus of the topological stratum of a given arbitrary orbifold eigenset, the more of a chance that such a tendency alone will then work to involve the resultant causation of oscillation-based distortions upon the said respective orbifold eigenset of topological stratum.  Therefore, the higher that the intensity of electromagnetic energy is, upon the proximal locus of the holonomic substrate of an orbifold eigenset of topological stratum is, the more likely that the correlative orbifold eigenset is to then to work to bear a higher tense of substringular abrasion -- since such an individually taken factor will tend to increase the tendency of working to form oscillation-based distortions upon the topological surface of the holonomic substrate of such a said respective given arbitrary orbifold eigenset --- if over the same duration of group-related metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Heat And Orbifold Abrasion

A given arbitrary orbifold eigenset is said to work to bear the tense of working to form either a cohomological generation and/or a cohomological degeneration, that is of an abrasive nature -- when there is a significant scalar amplitude and/or a significant scalar magnitude of oscillation-based distortion, that is to happen to the external fringes of the topological stratum of the Ward-Cauchy bounds of the holonomic substrate, that is of such a said respective given arbitrary orbifold eigenset, over a set group-related metric.  Such a so-stated abrasive Ward-Cauchy-based condition -- is often produced, when there is a relatively high scalar amplitude or a relatively high scalar magnitude of heat energy, that is applied to the proximal locus of the topological-based stratum of such a so-stated orbifold eigenset, -- as it is to be going through a correlative Fourier Transform.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Yau-Exact Superstrings And Cohomologies

Yau-Exact superstrings are called Yau-Exact, in part, because such superstrings of discrete energy permittivity are utilized to work to comprise orbifold eigensets -- that are considered here to be, in fact, Yau-Exact -- because such eigensets tend to generate as much of a scalar magnitude and as much of a scalar amplitude of cohomology-based topological stratum, as these tend to work to degenerate as such, -- over time.
Again -- an orbifold eigenset is a set of one or more discrete quanta of energy, that work or operate in so as to be performing one specific given arbitrary respective function, -- at the physical cite of their correlative Ward-Cauchy bounds.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cyclic Permutations Involving Ward-Supplemental-Based Paths

Let us initially consider an orbifold eigenset, that is to be traveling through an initially considered discrete Lagrangian-based path.  Let us say, that all of the sudden -- the said orbifold eigenset, is to be effected by the Chern-Simons-based condition of a Ward-Supplemental-based perturbation, upon the topological stratum of the holonomic substrate of the said orbifold eigenset.  This will then work to cause the said eigenset, to ensue at attaining an antiholomorphic Kahler condition.  Let us say that the said orbifold eigenset, is to be traveling through six spatial dimensions plus time, in this general respective given arbitrary case.  So, there are actually quite a number of possibilities as to what exactly are to be the arrangement -- of those respective complex roots, that are to here to be directly associated with the here resultant antiholomorphic Kahler-based Lagrangian path.  Let us next say, that the said eigenset is to then to reverberate back into one of its original parameters of homomorphism, in so as to then to work to attain an antiholomorphic Kahler-based condition, --  that may be attributed to it in the meanwhile.  This to, is to be associated with one of a number of a potential sets of arrangements of those respective complex roots, that are to here to be directly associated with the here resultant antiholomorphic  Kahler-based Lagrangian path.   Let us next consider this general genus of activity to repeat -- in an analogous but cyclical permutative manner -- to where, over a relatively spread-out group-metric, the same Lagrangian-based paths are Not to be identically mapped-out in the same fashion -- but in such a manner, to where there are here to be an iterative cycle of a set of similar but different combinations of complex roots, that are to work here in so as to help at working to form similar but different combinations of the resultant antiholomorphic Kahler-related Lagrangian-based paths.
 I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Nucleons And Spatial Dimensions

The individually taken mass-bearing superstrings of discrete energy permittivity, that work to make-up the nucleons of an atom -- tend to exist in what may be termed of as f-fields.  F-Fields exist in a minimum of four spatial dimensions plus time.  The holomorphic direction of such mass-bearing superstrings,  tends to be in the direction of the topological stratum of the external fringes of the core-field-density of those individually taken superstrings, that work in so as to help comprise the eigenstates of an f-field.  This would then work to help indicate, part of the condition as to why, orbifolds that are comprised of f-fields tend to exist in Fourier Transforms that work to include less spatial dimensions than either a neutrino, a photon, or an electron.  Since this would, as well, work to elude to the condition -- that the mass-bearing superstrings of discrete energy permittivity, that work to comprise a nucleon, act in so as to tend to move in the general direction of their width, -- then, this works to elude to the condition, when it comes to the correlative Fourier-Transforms that operate as is according to a Noether-based flow,  that the motion of the internal reference-frame of a nucleon will tend to be less aerodynamic than the motion of the internal reference-frame of a photon, over time.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Antiholomorphic Kahler Conditions And Gravity Waves

Often, a gravity wave -- of which is here to be that general multiplicit category of physical phenomenology, that exists as the kinematic expression of what may be deemed of here as Schwinger-Indices -- may be propagated in a back-and-forth manner along the topological-based stratum of the holonomic substrate of a compactified "collage" of mini-stringular segmentation, over the course of a set of metrical-based activity, that may be gauged here, as a Ward-Caucy-based example of a spontaneous Fourier-related activity of a substringular reverberation.  Let's take this from the "top."  A set of second-order light-cone-gauge eigenstates -- that are of the integrative plausible inter-relationship of the quantific characteristic of the overall light-cone-gauge eigenmatrix, that is of one discrete orbifold eigenset, are "plucked" like a harp by the directly corresponding gauge-boson eigenstates, in so as to help at working to form a discrete quantum-based characteristic of the correlative integration of the directly corresponding Schwinger-Indices, in so as to then act as those correlative interdependent set of gravity waves -- of which are to here be propagated along the proximal localized Rarita Structure eigenstates, in so as to help at working to allow for the basic Ward-Caucy-related condition, of physical phenomenology, to be able to then be able to work to bear a general multiplicit Yukawa-based coupling with other of such general physical-based phenomenology, over a sequential series of group-related instantons.  Let us next, consider that general condition, of a given arbitrary respective orbifold eigenset, of which is to reverberate in a back-and-forth manner, in so as to pushed from one general relative forward-holomorphic-based direction, into then being pushed into then going into the opposite general holomorphic direction, while then being pushed back into the initially said relative forward-holomorphic direction, while then being pushed back into the relative reverse-holomorphic direction, and so on.  Each time that what was here to be considered as a reversal in what is to then be the forward-holomorphic direction, there is to then be a series of ensuing antiholomorphic Kahler conditions.  This will then work to help at forming an ensuing series of what is to tend to here be a closely-knit tense of Kahler-Metric eigenstates.  As the said respective orbifold eigenset is to reverberate, in so as to help at working to form what will here be a sequential series of Kahler-Metric eigenstates, -- the resultant effect that this is to then occur upon the holonomic substrate of the proximal localized Rarita Structure eigenstates, will then tend to form a tense of one or more reverberation-based rippling effects, upon a set of one or more compactified eigenstates of mini-stringular  segmentation, in so as to help at working to form a back-and-forth set of Fourier-related vibrational oscillations, that will then act as gravity waves -- that are to be propagated between the ends of the holonomic substrate of two different topological stratum.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.