As To Charge

 Charge amounts to being --- The kinematically distributed delineation, of the wave-tug of magnetism-related metric-gauge eigenstates.  TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. 

The Proximal Local Presence Of Magnetism -- Induction Of Homomorphic Field

 The proximal local presence of a relatively enhanced scalar amplitude of magnetism, at times, may often work to induce a physically latent Hamiltonian Operator, to spontaneously become isotropically stable, -- to where it will thereby tend to spontaneously ensue, in so as to work to bear the proximal local presence, of a homomorphic field, -- to where such a stated Hamiltonian Operator, may often tend to consequently ensue, in so as to work to spontaneously exhibit the display, of a tense of group action. SAM ROACH.

Escalating Flow Of Spatial Transference And Magnetism

 Let's say, that one were to initially have two relatively analogous Hamiltonian-Related fields. One of such fields, is here to work to bear an escalating flow of spatial transference, while the other of such fields, is not to work to bear such a tense of escalation, in its correlative spatial transference. That respective Hamiltonian-Related field of the two, of which is to work to bear the earlier mentioned escalating flow of spatial transference, will often tend to work to exhibit the display, of a greater scalar amplitude of magnetism. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH. 

Homotopic Dispersion -- Riemann/Rayleigh Scattering

 When a given arbitrary tense of homotopic dispersion is to happen, via a Riemann Scattering, this will often have the general tendency, of working to form magnetism, of which will tend to reverse-fractal into electrodynamic charge.  Whereas; When a given arbitrary tense of homotopic dispersion is to happen, via a Rayleigh Scattering, this will often have the general tendency, of working to form a local tense of holonomic disorder, of which will tend to reverse-fractal into entropy. TO BE CONTINUED! SAMUEL.

Dispersed Homotopic Residue — Correlative Scalar Amplitude Of Magnetism

 The stronger that the dispersive “thrust” is to be, of a consequentially scattered set of harmonic eigenstates of homotopic residue, the greater that the directly associated resultant generative force of magnetism will therefore tend to be. I WILL CONTINUE WITH THE SUSPENSE LATER! SAM.

What Magnetism Is

 Homotopic Residue tends to be the holonomic metric-gauge-related phenomenology, of the output of perturbative Chern-Simons Invariants. The general effect of harmonically scattered homotopic residue upon cohomology, tends to work to form magnetism. I WILL CONTINUE WITH THE SUSPENSE LATER! SAMUEL DAVID ROACH.

Magnetism -- Braided Cohomology

 The greater the scalar amplitude of magnetism, that a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, is here to exhibit, the more likely, that such a stated Noether-Based mass-bearing cohesive set of discrete energy quanta, is thence to tend to work to exhibit the display, of a tense of a braided cohomology. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAMUEL.

Highly Magnetic Current -- Tightly Braided Cohomology

 The greater that the scalar amplitude of the magnetism is to be, for an electrodynamic current, the more tightly braided, that the directly associated superstring-related cohomology will tend to be. Samuel Roach.

High Scalar Amplitude Of Magnetism Applied -- The More Braided The Cohomology

 The higher that the scalar amplitude of a tense of magnetism is to be, that is here to be directly applied upon the topological manifold, of a spinning mass-bearing cohesive set of discrete energy quanta, -- that is here to be working to bear a recursively smooth Ricci Flow -- the more tightly braided that the directly corresponding cohomology will tend to result in displaying, over a correlative respective time period. SAM.

Isotropic Stability And Magnetism

 Molecular lattices that are here to be comprised of, by many cohesive sets of isotropically stable mass-bearing discrete energy quanta -- tend to bear a greater scalar amplitude of magnetism, than other types of molecular lattices, that are not to be comprised of as such. To Be Continued! Sincerely, SAM ROACH.

A Charged Diffeomorphic Field

 A charged diffeomorphic field tends to work to form a more harmonic tense of magnetism, than a similar charged field, that is, instead, to not work to bear a diffeomorphic geometry. Sincerely, SAM ROACH.

Electrons — As To Being Gliosis To The Kahler-Metric

 Since the electrons of any given arbitrary atom, tend to spin around the nucleus of such an atom; while, at an internal reference-frame,  the respective nucleus of such an inferred individually taken atom, is relatively stationary, in comparison to the earlier stated electrons, — those cohesive sets of discrete energy quanta, that are directly associated with the proximal local presence of the electrons of any given arbitrary atom, tend to bear a greater attribute, of acting as being Gliosis to the Kahler-Metric, than those cohesive sets of discrete energy quanta, that are directly associated with the proximal local presence of the respective nucleons, are to tend to exhibit. This is associated with part of the reason, as to why electrons are more heuristically thought of, in terms of what is more responsible for the causation of the generation of magnetism, than the otherwise considered role that nucleons are to bear, instead  — when in terms of the generation of magnetism. I will continue with later! To Be Continued! SAMUEL DAVID ROACH.

Some Stuff As To Being Gliosis ToThe Kahler-Metric

 The more rapidly that a given arbitrary mass-bearing cohesive set of discrete energy quanta, is to undergo the general processes of working to bear anti-holomorphic Kahler conditions — the more that such a said set of discrete energy quanta, will consequently tend to bear the characteristic, of being Gliosis to the Kahler-Metric. Therefore; the more that a mass-bearing cohesive set of discrete energy quanta, is to work to bear the characteristic of being Gliosis to the Kahler-Metric, the more likely that such a said set of discrete energy quanta, — will tend to work to externally bear,  a relatively higher scalar amplitude of a tense of magnetism. I will continue with the suspense later! To Be Continued1 Sincerely, SAM ROACH.

Proximal Local Presence Of Kahler-based Quotients

 The proximal local presence, of what works to form that general holonomic substrate, that may be mathematically described by the conceptualization of Kahler-based quotients, as this is here to be appertaining to the multiplicity of the metric-related condition of discrete energy phenomenology, helps to work to form a basis, for the existence of magnetism. I will continue with the suspense later! Sincerely, SAM ROACH.

Group Action And Magnetism

 Let us initially consider two different unique mass-bearing cohesive sets of discrete energy quanta.  Both of which are here to be of the same quantum of mass; as well as the given arbitrary physical condition, that both of such said sets of discrete energy quanta, are, as well, to work to bear the same innate tendency of working to exhibit a De Rham cohomology.  Furthermore; both of such respective mass-bearing cohesive sets of discrete energy quanta,  are also to tend to work to bear both the same charge, as well as working to bear the same basic means, of translating the exhibition of the externalized transversal component of their Fourier-related spatial delineation, over a fairly transient covariant relativistic duration of time, that is here to be simultaneous in comparison to one another — as this is to occur, via the vantage-point of a central coni-point.  The main difference in the behavior of these two said cohesive sets of discrete energy quanta, is that one of such sets of cohesive discrete energy, is to bear a reductional tense of group action — by working to bear a tense of isotropic stability; whereas, the other of such said respective given arbitrary mass-bearing cohesive sets of discrete energy quanta, is to work to bear a tense of isotropic instability. That stated set of discrete energy quanta (mass-bearing cohesive set), that is here to be of a tense of isotropic stability, will tend to result in working to display a relatively higher scalar amplitude of a fractal of magnetism, than the other of such said mass-bearing cohesive sets of discrete energy quanta, — of which, instead, is consequently to result in working to bear a lower scalar amplitude of a fractal of magnetism. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

As To Vibrational Delineation

 Let us initially consider a mass-bearing cohesive set of discrete energy quanta, that is here to be changing in its tense of relative motion, when this is here to be taken, in its relationship to the motion of electromagnetic energy. The net resultant vibrational delineation of the i*PI(del) Action --  of which is here to be correlative to that respective given arbitrary attribute of the self-same stated i*PI(del) Action, that is here to be directly corresponding to the integrable summation, of which is of the net attribute of those individually taken superstrings of discrete energy permittivity, that are here to work to comprise the topological manifold-like structure, that is of the inferred cohesive set of discrete energy quanta, -- tends to work to act as a key factor, in the formation of those perturbative Chern-Simons Invariants (of which are otherwise, to only remain as "Invariant," if the said respective cohesive set of discrete energy quanta is to maintain a constant tense of relative motion, when this is here to be taken in relation to the motion of electromagnetic energy), to where this is to tend to reverse-fractal into a tense of magnetism. SAM ROACH.

As To The Level Of Increment, Of Lorentz-Four-Contraction

 Initially: Please keep in mind, that Chern-Simons Invariants are only "invariant," when/if the motion of a cohesive set of discrete energy quanta, in any given arbitrary case scenario that is correlative to any set situation, is not to be changing at all, in its relationship to the motion of electromagnetic energy. The more that the gauged-action-related perturbation, that is here to be of a tense of the alteration of those correlative Chern-Simons Invariants, that are thence to be most appertaining to a tense of the fluctuation of the motion of a mass-bearing cohesive set of discrete energy quanta, is to work to display the general tendency, of a heightened scalar increment of a tense of a Lorentz-Four-Contraction, -- the more that there will be a higher probability, of a resultant consequential tendency of the proximal local presence, of the cohomology-related generation, of which will consequently tend to reverse-fractal, into the result, of an increase in the directly corresponding scalar amplitude, of the amount of magnetism, that such a stated cohesive set of discrete energy quanta, will thereby tend to be exhibiting. Consequently, as the corollary to the just mentioned idea; The less that the gauged-action-related perturbation, that is here to be of a tense of the alteration of those correlative Chern-Simons Invariants, that are thence to be most appertaining, to a tense of the fluctuation of the motion of a mass-bearing cohesive set of discrete energy quanta, is to work to display the general tendency, of a lowered scalar increment of a tense of a Lorentz-Four-Contraction, -- the more that there will be a higher probability, of a resultant consequential tendency of the proximal local presence, of the cohomology-related de-generation, of which will consequently tend to reverse-fractal, into the result, of a decrease in the directly corresponding scalar amplitude, of the amount of magnetism, that such a stated mass-bearing cohesive set of discrete energy quanta, will thereby tend to be exhibiting. Furthermore; when the i*PI(Del) Action is to work to bear a tendency, of a decrement of what I term of as being the phenomenology of "partition-based discrepancies," per each individually taken superstring of discrete energy permittivity, that is here to work to comprise its respective mass-bearing cohesive set of discrete energy quanta, this said general tendency, will tend to work to bear a kinematic activity, which will indirectly work to help at forming the homotopic product, of the gauged-action, of a discrete quantum of cohomology-related generation, with the gauged-action of a discrete quantum of group-related instanton. This results in a general tense of a reverse-fractal, that tends to work to form an increase in the scalar amplitude, of the proximal local magnetic field. Consequently; when the i*PI(Del) Action is to work to bear a tendency, of an increment of what I term of as being the phenomenology, of  "partition-based discrepancies," per each individually taken superstring of discrete energy permittivity, that is here to work to comprise its respective mass-bearing cohesive set of discrete energy quanta, this said general tendency, will tend to work to bear a kinematic activity, which will indirectly work to help at forming the homotopic product, of the gauged-action of a discrete quantum of a cohomology-related de-generation, with the gauged-action of a discrete quantum of group-related instanton. To Be Continued! Sincerely, Samuel David Roach.

Magnetism And Isotropic Stability

 Let us initially consider a charged mass-bearing cohesive set of discrete energy quanta. The more isotropically stable that such a said cohesive set of discrete energy quanta is to be, the more that it will tend to exhibit a tense of magnetism.  Consequently; the less isotropically stable that such a said cohesive set of discrete energy quanta is to be, the less that it will tend to exhibit a tense of magnetism. SAM ROACH.

Orbifold Eigensets, Charge, And Rapid Cycling

Orbifold eigensets that work to bear a Majorana-Weyl-Invariant-Mode, that is to behave at the quantum level -- in so as to bear a relatively high scalar amplitude, as to working to bear a rapid cycling of going back-and-forth -- from generating cohomology-based eigenstates to degenerating cohomology-based eigenstates, and so-on, -- often tend to bear at least some sort of magnetic-related attraction to other orbifold eigensets, that work to bear a Majorana-Weyl-Invariant-Mode that, instead, is to behave at the quantum level -- in so as to bear a relatively low scalar amplitude, as to working to bear more of a gradual cycling -- of going back-and-forth, from generating cohomology-based eigenstates to degenerating cohomology-based eigenstates, and so-on.  I will continue with the suspense later!  To Be Continued!  Sam Roach.

More Info About The Kahler-Metric

Let us say that there is here to be the presence of a set of one or more antiholomorphic Kahler conditions -- in so as to begin what is here to be the ensuing proximal presence of a Gliosis-related tense, of the Kahler-Metric to transpire here.  Once that the said antiholomorphic Kahler-conditions are here to be taking place, over a transient duration of time -- there is then to ensue, the proximal local presence of a Wick Action eigenstate.  The ensuing kinematic motion of the just mentioned Wick Action eigenstate, is then to work to produce a potentially repelling distribution of the proximal local homotopic residue, -- which will then help to work to form a change in the consequent delineation of both the local group-attractors and the local ghost-inhibitors.  This alteration in the delineation of both the local group-attractors and the local ghost-inhibitors, will consequently result in helping in the Ward-Cauchy-related condition -- of working to allow for the right genus of both cohomological generation and cohomological degeneration -- in so as to work to help in potentially working to alter the fractal-based tense of the magnetic field, that the correlative so-eluded-to orbifold eigenset is then to begin to attain.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.