Parity Between Adjacent Scattered Eigenindices

Let us initially consider a cohomological pattern, that had just formed at one given arbitrary locus.  Let us next consider this said cohomological pattern, as a "snapshot" in the substringular -- as being of a Laplacian-related Ward-Cauchy case scenario.  Let us now consider that the norm-state-projections that an orbifold eigenset had acted upon here -- in so as to work to form the said cohomology -- had formed what may be termed of as a Reimman scattering to a respective extent, in so as to form the so-eluded-to generation of cohomology eigenstates.  Now, let us consider two of the eigenindices that have here to have just been formed by the said cohomological generation -- in such a case in which these two respective given arbitrary eigenindices, which are out of the much larger overall Hodge-Index of the overall cohomological phenomenology of such a respective given case, are here to be adjacent to one another, at the proximal locus of the correlative Laplacian Transform.  These two adjacent scattered eigenindices, are of a Reimman scattering -- to where these are to bear an even parity.  This then works to elude to the Ward-based condition, that, if one were to theoretically fold together the two different individually taken eigenindices at their central coniaxion towards one another -- this would work to form a general genus of an isomorphic symmetry, at the point of duration of the correlative "snapshot" of time.  I will continue with the suspense later!  To Be Continued!
 Samuel David Roach.

More Stuff As To Cohomological Generation, Voltage

Let us initially consider an electron -- that is to be smoothly transferred in a metrical-related manner, through a given arbitrary initial medium over time.  Let us then say that the said respective electron, is to initially be smoothly generating cohomology over time.  Let us next say that the medium in which the said electron is to be translated through is to change in its molecular composition -- into a medium that is here to bear an ensuing stronger electrical resistance, -- in spite of the condition that such a so-stated electron is to here to continue to generate cohomology at the same rate per time.  This will then mean -- that the electron is to now to bear more energy per cohomological generation, over time.  This will furthermore mean -- that the electron is to now to bear more energy per generation of charge, over time.  This will then mean, that the said electron will consequently work to bear more voltage -- as it is here to maintain its charge per time -- in the process of going through more of a scalar amplitude of electrical resistance over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two About Electrons And Cohomological Generation

Let us initially consider an electron -- that is here to be accelerated through a given arbitrary conductive cable, as a metrical-gauge-related Hamiltonian operator, that is to be propagated through its respective Hamiltonian operand -- along the trajectory of its correlative Lagrangian-based path, over an evenly-gauged Hamiltonian eigenmetric.  Let us next consider, that the conductance of the material that is here to work to comprise the general magnetism, in which the said electron of this respective case is to be tugged into an electrical flow -- by the translation of the activity of its valence bands -- is to increase in its scalar magnitude, over the Fourier Transformation in which the electron is to go through the process of being transferred through the said respective Hamiltonian operand, in a manner that is Lagrangian-wise hermitian over time.  Since the said electron is here to be accelerated -- the pulse of that just mentioned electron will be amplified in a Ward-Cauchy-related manner, along the course of the propagation of the said electron across its correlative valence bands.  This will then work to indicate, that this will then involve a set of metrical-based Chern-Simons singularities.  As this is to occur, let's say that things happen, to where the acceleration of the said electron is to be maintained in its scalar translation over time, -- in spite of the added conductivity.  This will then work to cause an increase in the generation of its charge over time, -- and thus, this will then work to cause an increase in its cohomological generation over time.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Some Additional Stuff About Cohomological Generation, I

Let us consider a discrete superstring of discrete energy permittivity, that works to move through a discrete Lagrangian path over time.  The said superstring is here to be interacting in a Gliosis-related manner, with those norm-state-projections that are in its immediate path -- in the process of moving through the Hamiltonian operand that is amidst of its said Lagrangian-related path.  Such so-stated projections, are here to be scattered upon their direct contact.  These said norm-state-projections are either to be scattered in a harmonic manner, or, in an enharmonic manner -- over the directly corresponding sequential series of group-related instantons.  A scattering at the Ward-Cauchy-related level, is said to be of a Reimman-related manner -- if the adjacent displaced eigenindices are said to have an even parity.  Furthermore -- a scattering at the Ward-Cauchy-related level, is said to be of a Rayleigh-related manner -- if the adjacent displaced eigenindices are said to have an odd parity.  If the said scattering is of a Reimman-related manner -- the directly corresponding scattering is said to be of a harmonic nature.  Yet, if the said scattering is of a Rayleigh-related manner -- the directly corresponding scattering is said to be of an enharmonic nature.  When a Ward-Cauchy-related scattering is of a Reimman-related nature -- it is said to be generating cohomology. Yet -- when a Ward-Cauchy-related scattering is of a Rayleigh-related nature -- it is said to be degenerating cohomology.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel Roach.

Electrons And Cohomological Degeneration

If any one given arbitrary electron, is to decelerate in the course of working to travel through any one given arbitrary medium over time -- such a respective electron, will  consequently tend to degenerate in charge per time.  Such a degeneration of charge per time, is here to correspond to a degeneration of cohomology per time.

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

Electrons And Cohomological Generation

As any one given arbitrary electron, is to be accelerated through one given arbitrary medium over time -- such a said respective electron, is to then to work to generate charge over time.  As an electron is to generate charge over time -- it is to then to be generating cohomology over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cohomological Degeneration And Melting

Let us initially consider one relatively large set of orbifold eigensets -- that work to form a molecule.  Each individually taken orbifold eigenset -- that works to help at comprising the said molecule -- is a set of discrete quanta of energy, that operate in so as to perform one given arbitrary function.  The overall set of orbifold eigensets, that work to comprise the said molecule, is of that state of condition, -- to where the said molecule is initially a solid.  There is here to be a relatively small scalar magnitude of infrared energy or heat, that is here to be directly interacting with the said molecule -- to where the said molecule is here said to be frozen, in so as to be a solid.  As the temperature of the molecule of this case is to increase -- this corresponds to the condition that there is here to be a correlative increase in the amount of heat or infrared energy, that is to be directly being applied to the said molecule per time.  Heat is a form of electromagnetic energy, since it is infrared electromagnetic energy.  So, as the amount of heat that is being applied to a region is to increase per time, -- there is to here be an increase in infrared electromagnetic scattering to be applied to the proximal locus of the said molecule per time.  As there is here to be a multiplicit increase in the Ward-Cauchy condition of infrared electromagnetic energy, that is to be applied to a set proximal locus over time -- there it to be an increase in the scalar amplitude of the density of the correlative entropic photons over time.  This eludes to an increase in the proximal local density of entropy, that is here to be produced in a set region per time.  Entropy is disorder.  An increase in the disorder or entropy -- that is here to be directly associated with the Ward-Cauchy condition of the overall interaction of the orbifold eigensets, that work to comprise a molecule, -- works to interact with the earlier mentioned condition of an increase in the scalar amplitude of heat energy, that is at a proximal locus over time, in so as to help at working to allow for that respective molecule to melt.  The earlier mentioned Ward-Cauchy condition of an increase in the regional entropy per time, works to degenerate certain aspects of the cohomological index of that molecule that is here to be melting -- due to the combined effects of both an increase in heat per time, and, an increase in entropy per time, in a given set region.  So, the melting of a molecule -- is partially due to the consequent overall cohomological degeneration of a relatively large set of orbifold eigensets -- that work to help at comprising the proximal local region of a molecule.  Melting is then as well, in part, due to the local decrease in the Majorana-Weyl-Invariant-Mode, that is of a conformally invariant set of orbifold eigensets -- that is at the internal reference frame of the set molecule, when this is taken as one overall whole.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

As To Electromagnetic Energy And Cohomological Generation

Let us initially consider a photon that is colliding with an electron, that is of one given arbitrary atom.  The said electron is situated here at the relative external energy level or valence shell of the directly corresponding atom, that is here being discussed.  As the so-mentioned photon is here in the process of scattering upon the correlative electron -- the photon is here to temporarily become entropic, while the electron that is here to be collided into in a Gliosis-based manner, is to consequently jump back-and-forth an energy level, -- in so as to then to undergo the Fujikawa Coupling, to where the said electron is to result in working to release its spare discrete kinetic energy in the form of a photon (in the form of a discrete quantum of electromagnetic energy).  The earlier mentioned photon, that had just scattered upon the so-stated electron, in so as to become entropic -- is then to degenerate cohomology -- in the process of rebounding from an initial Rayleigh-related scattering, back into subsequently re-quantizing into the Hamiltonian operand of the respective general beam of electromagnetic energy -- that is proximal local to the so-eluded-to electromagnetic permeation of the Ward-Cauchy-related region, in which the electromagnetic energy is here to be scattering within.  During the course of the same general evenly-gauged Hamiltonian eigenmetric, the process of the Fujikawa Coupling, -- in which the electron that was just struck at the externalized core-field-density of its correlative light-cone-gauge eigenstate, is so as to release its residual spare discrete kinetic energy into a photon, -- is to work to generate cohomology.  Consequently, the scattering of light works to both degenerate cohomology in one genus of manner, while also working to generate cohomology in a different genus of manner -- as the correlative discrete quanta of electromagnetic energy is sprung upon the holonomic substrate of a mass-bearing discrete quanta of energy, in a Gliosis-based manner over time.  This is here to be a balance, that is here to be formed between that general Hamiltonian operation of entropy, that works to degenerate both cohomological eigenstates and cohomological eigenindices, -- and that general Hamiltonian operation of electromagnetic induction, that works to generate both cohomological eigenstates and cohomological eigenindices, over time.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Infrared Energy

Let us initially consider a set of orbifold eigensets, that operate cohesively in a Ward-Cauchy-related manner -- that is both covariant, codeterminable, and codifferentiable over time.  The more infrared energy or heat that is here to be applied to the one given arbitrary set of orbifold eigensets of such a case -- over any proscribed set evenly-gauged Hamiltonian eigenmetric -- the less tightly that the correlative Majorana-Weyl-Invariant-Mode will tend to be, of the respective said set of the correlative orbifold eigensets.  Consequently, the less infrared energy or heat that is here to be applied to any one given arbitrary set of orbifold eigensets over any proscribed set evenly-gauge Hamiltonian eigenmetric -- the more tightly that the correlative Majorana-Weyl-Invariant-Mode will tend to be, of the said set of the correlative orbifold eigensets.  This is due to the condition, that heat that is pulled away from a Ward-Cauchy-related proximal local region, will tend to decrease the correlative scalar amplitude of the correlative molecular vibrational oscillations, and thereby work to increase the scalar amplitude of the correlative Majorana-Weyl-Invariant-Mode -- whereas, heat that is pulled into the physical bounds of a Ward-Cauchy-related proximal local region, will tend to increase the correlative scalar amplitude of the correlative molecular vibrational oscillations, and thereby work to decrease the scalar amplitude of the correlative Majorana-Weyl-Invariant-Mode.  This general genus of a means of either a correlative decrease in proximal local infrared energy -- or a correlative increase in proximal local infrared energy -- works to imply the general application, of the process of convection, to the eigenstates that are here to be of an internal Ward-Cauchy-related reference frame, -- that is at the Poincare level to the topology of the external shell, that is of the here correlative inherent multidimensional stratum of the directly corresponding molecular structure, of this generic means of a case scenario, over a relatively transient set of comparative time periods.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Net Resultant Complex-Roots

Let us initially consider a mass-bearing set of discrete energy quanta, that works here to comprise one given arbitrary orbifold eigenset -- of which is here to exist in a state of a Majorana-Weyl-Invariant-Mode.  Let us next consider the correlative set of those complex-roots -- that are here to be directly associated with the Lagrangian-based Chern-Simons singularities, that are formed in the process of the here latent antiholomorphic Kahler conditions, that are here to be directly associated with the relatively continuous flow of that correlative Ward-Supplemental wave-tug, by which the said orbifold eigenset is here to continuously rebound from within the Ward-Cauchy-related constraints of the said Majorana-Weyl-Invariant-Mode.  Next, let us say that one were here to take the resultant summation of the earlier mentioned complex-roots -- that are here to be directly associated with the earlier mentioned Lagrangian-based Chern-Simons singularities.  Both the scalar amplitude and the directoral-related holomorphicity of those said complex-roots, of such a respective said case, that are not nullified in any one of such a given arbitrary respective case, would here work to indicate to a certain extent -- the eigenindices of both the relative direction and the scalar amplitude of the resultant vibrational oscillations, that are of the resultant relatively superconformally invariant orbifold eigenset, that is of such a given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Complex Roots

Let us consider an initial situation -- in which one is here to be considering a set of mass-bearing superstrings, that are here to be existent under a condition of a tightly-knit Ward-Cauchy-based state of Majorana-Weyl-Invariance.  Let us next consider the condition, that there is here to be a constant state of a reiterative set of antiholomorphic Kahler conditions -- in which there is to be a relatively continuous state of the formation of Lagrangian-related Chern-Simons singularities.  The relatively tighter that the scalar amplitude is -- as to the condition of the correlative Majorana-Weyl-Invariant-Mode -- the more that there is to be the tendency, of those complex-roots that are thence to be indicatively formed by the earlier mentioned Lagrangian-related Chern-Simons singularities, to add-up to a resultant of basically zero, -- at the reference-frame of the proximal locus of the Ward-Cauchy-based region, of which is at the Poincare level to the external shell of so-eluded-to mass-bearing orbifold eigensets, of which are here to be undergoing that correlative Fourier Tranformation, in which the so-eluded-to set of discrete energy quanta have here to be going through the general activity of a Ward-Cauchy-based condition of a substringular-related "homoestasis" over time.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Majorana-Weyl-Invariant-Mode And Cohomological Generation

The higher that the scalar amplitude is to be, that is of the correlative Majorana-Weyl-Invariant-Mode -- the more Yau-Exact will be the tendency of the directly corresponding orbifold eigensets, that will here work to then be comprised of by the overall set of mass-bearing discrete energy quanta, to where this will then operate in so as to work to comprise a mass, that is here to be directly correlative to the respective given arbitrary Ward-Cauchy-related case scenario of this given genus of situation.  The more Yau-Exact that a set of mass-bearing discrete quanta of energy will tend to be, -- the more acutely that the so-eluded-to set of discrete energy quanta will then tend to generate as much cohomology as it will tend to degenerate over time.  This will then mean, that -- the more Yau-Exact that a set of orbifold eigensets will tend to behave as portraying -- the more piece-wise continuous that such a set of discrete energy quanta that operate in so as to perform one common function, will tend to generate as much cohomology as it will tend to degenerate over time.  Therefore, any set of orbifold eigensets, that operate in so as to be able to bear a relatively high resonant vibration -- will tend to acutely generate as much cohomology as it will degenerate -- as a piece-wise continuous Hamiltonian operator -- as well as that such a Hamiltonian operator, will tend to bear a relatively high scalar amplitude of a Majorna-Weyl-Invariant-Mode, over any one proscribed evenly-gauged Hamiltonian eigenmetric.  I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.

Majorana-Weyl-Invariance And Resonant Vibration

Let's say that one were here to be dealing with mass-bearing discrete quanta of energy.  The higher that the Majorana-Weyl-Invariant-Mode is -- at the reference frame of the proximal locus of the directly corresponding orbifold eigensets, that are here to work to be comprised of by the respective given arbitrary mass-bearing discrete quanta of energy of such a given case -- the higher that the directly corresponding resonant vibration will tend to be of that mass, that is here to work to be comprised of by the said respective correlative orbifold eigensets.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Ghost-Inhibitors And Rayleigh Scattering

Let us initially consider an orbifold eigenset -- of  which is here to be traveling through a discrete Lagrangian path -- via a Hamiltonian operand, that is in the course of the trajectory of the respective motion of the said orbifold eigenset -- as the so-eluded-to set of discrete quanta of energy that operate in so as to perform one specific function, is undergoing an evenly-gauged eigenmetric over time.  This said eigenset is here to tend to be working to form a De Rham cohomology, over a sequential series of group-related instantons.  This will then mean that the here correlative orbifold eigenset, is to be both metric-wise and Lagrangian-wise completely hermitian -- when one is here to consider the overall net resultant pulsation and path-based flow of the so-eluded-to set of discrete quanta of energy, over the proscribed gauged-metric.  Since the respective orbifold eigenset is here to be both coherent and of a Noether-based flow over time -- the directly corresponding composition of the said orbifold eigenset, is to tend to act here as a composite structure -- that is both unified and of a covariant given tense of a Majorana-Weyl-Invariant-Mode.  Let us next say that a ghost-inhibitor is to then to work to interfere with the translation of the generation of both the formative cohomological eigenindices and the formative cohomological eigenstates, that are here to be formed by the consequential result of the interaction of the inherent correlative discrete quanta of energy with the proximal local flow that these bear upon their immediate environment.  The more Yukawa that such an interference is to be, over the said evenly-gauged-metric, the more that such an iterference will tend to have the potential of working to form a Rayleigh scattering -- of the eigenmembers of the discrete quanta of energy that are of the composition of the orbifold eigenset, from each other, -- to where those eigenstates of discrete energy that had initially to have worked to help at the formation of the said orbifold eigenset, may then scatter away from one another -- in so as to work to dissolve both the structural and the functional operation of the said eigenset,  from its initial conditions of both its Ward-Cauchy-related construction and its Ward-Cauchy-related interaction-based mode of activity. 
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Njenhuis Wobble Of Superstrings

As superstrings of discrete energy permittivity that are here to be in the process of group-related instanton, in which these are here to be working to bear their relatively mild vibrational oscillation, during the course of any one specific iteration of BRST -- these individually taken discrete quanta of energy permittivity, are here to work to bear a side-to-side wobble, as taken from their relative Njenhuis-to-forward-holomorphic side to their relative Njenhuis-to-reverse-holomorphic side -- in such a manner, to where such a so-eluded-to general genus of wobble is to tend to be subtended at a relative angling of ~1.104735878*10(-81)i degrees.  (Such a so-eluded-to general genus of wobble is to subtended at a relative back-and-forth angling of ~1.104735878*10^(-81) degrees.  As this is to be happening -- such a directly pertinent given arbitrary respective discrete quantum of energy permittivity, is to be simultaneously going through both the Polyakov Action and the Imaginary Exchange of Real Residue, via the vantage-point of a central conipoint.  (See my past writings for more of as to what I mean by this.)
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As To The Leverage Of The Higgs Action

The leverage of the Higgs Action, is caused primarily -- due to the leverage of the Fischler-Suskind Mechanism.  The general multiplicit condition of the Fischler-Suskind Mechanism, is comprised of by a correlative set of norm-state-projections, that work to bear a consequent orthogonal relationship -- that works to bear a wave-tug-related leveraging of ~6.25*10^18 (which is the reciprocal of the scalar magnitude of the smallest tense of discrete charge, which is ~1.6*10^(-19)Coulumbs) upon the correlative multiplicit Higgs Action eigenstate -- in so as to work to bring the activity of a Gliosis-related relationship, that is to ensue between discrete energy and the here directly corresponding multiplicit eigenstate of the holonomic substrate of the Klein Bottle, via the Kahler-Metric, in so that such a general tense of a Fourier-Transformation is here to be brought into the process of working to allow for the said multiplicit discrete quanta of energy to here to be re-attaining their fractals of discrete energy, in so as to work to allow for discrete quanta of energy to both persist and exist over time -- via such a relationship of a correlative general tense of a Gaussian Transformation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Zero-Norm-State-Projections Causing Fujikawa Coupling

The general manner by which zero-norm-projections work to help at forming the general activity of the Fujikawa Coupling, is by the manner by which that the directly corresponding zero-norm-state-projection or projections -- that are here to act in so as to be bending the discrete quantum of kinetic energy permittivity in a hermitian manner, is acting in such a manner by which it is here to be arcing gradually although spontaneously in a hermitian manner -- via its correlative tense of a fractal of spin-orbital-momentum.  Here.  A given arbitrary set of one or more zero-norm-state-projections are to work to bear a wave-tug upon a discrete quantum of kinetic energy permittivity, that is to be subsequently released as the excess residual energy of an electron, in the form of a photon.  As such a said set of one or more zero-norm-state-projections are to bear a Gliosis-related Yukawa wave-tug -- upon the said discrete quantum of residual energy, the so-stated set of projections is then to work to bear a smoothly-curved torsioning upon the converting discrete quantum of energy -- in a manner that works to consequently smoothly bend the discrete kinetic energy that is then to be becoming discrete electromagnetic energy, in a manner that works to involve only as many changes in derivatives as the number of spatial dimensions that it is here to be traveling through, over its directly corresponding Fourier-Transformation.  It is the smooth translation of the fractal of spin-orbital-momentum -- that the here torsioning set of one or more zero-norm-state-projections are to be undergoing over time -- that is here to work to cause the consequent smooth translation of the hermitian bending of the here released kinetic energy of the corerlative electron, that is here to then ensue, in so as then to form a resultant photon (a photon is a discrete quantum of electromagnetic energy).
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Group-Attractors And Norm-State-Projections

Norm-State-Projections may often act -- in so as to produce a general tense of a wave-tug, of which may act as a very general genus of a group-attractor.  Such a general tense of a group-attractor, may then work to act -- in so as to delineate discrete quanta of energy, into the general form of an orbifold eigenset.  This is if the topological stratum, that is here to be both covariant, codeterminable, and codifferentiable between those discrete quanta of energy, that are here to be tugged together, -- is to be having either an increasing scalar magnitude or an increasing scalar amplitude of a general Yukawa-related bonding.  Such an increase in either the scalar magnitude or the scalar amplitude of a general Yukawa-related bonding, may often be related to a correlative Real Reimman relationship, that is to exist between the correlative complex-roots that these are to bear -- among their Lagrangian-based Chern-Simons singularities -- that these initially individually taken discrete quanta of energy had worked to form, immediately prior to the Fourier-based activity of the said norm-state-projections that are here to act as a group-attractor, that are here to have had acted upon the earlier mentioned discrete quanta of energy, that are here to subsequently bond at the relatively proximal locus of one discrete orbifold eigenset.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As To The General Way Group-Attactors Act

Superstrings that are to be brought together, in so as to operate to perform one specific function -- are brought into an eminently Yukawa Coupling, by the Fourier-related activity -- of what may here be termed of as group-attractors.  I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.

Adjacent Assymetric Orbifold Eigensets

Let us initially consider two different orbifold eigensets, that are immediately adjacent.  Let us next say that both of the individually taken orbifold eigensets, are to here to be undergoing a tense of Majorana-Weyl-Invariance at the "time."  Let us next say, that one were to extrapolate -- in so as then to compare   - the tense of the antiholomorphic Kahler conditions of the superstrings that are here to comprise one of the here given arbitrary orbifold eigensets, to the antiholomorphic Kahler conditions of the superstrings that are here to comprise the other given arbitrary orbifold eigenset, that is of this respective case.  In the process of such an extrapolation, one would here to be comparing those complex roots that are to here to be directly associated with both the Lagrangian-based Chern-Simons singularities and/or the metrical-based Chern-Simons singularities, that are to be formed via the interaction of the composite discrete quanta of energy of the two individually taken orbifold eigensets, as these are here to be undergoing a Fourier Transform, over a discrete amount of time.  Let us next say that the vibrational oscillation of the two here comparitive orbifold eigensets, is to be of an assymetric-based nature.  This will often mean, that the comparitive complex roots of their Lagrangian-based Chern-Simons singularities may then tend to be Njenhuis to one another -- during the said Majorana-Weyl-Invariant-Mode.  Sincerely, Samuel David Roach.

More About Discrete Residual Energy Released As Photon

As I have mentioned before, and as it is quite already known in physics -- when electromagnetic energy is to strike an electron, the said electron is here to have a tendency of jumping back-and-forth energy levels, in so as to release its residual kinetic energy in the form of a photon.  As the just mentioned photon is in the process of being formed by the so-stated released residual kinetic energy of an electron, -- the directly corresponding electron that is here to be moving back-and-forth an energy level, in the process of indirectly working to form a discrete increment of light, that is in the form of an impending photon -- (the said electron) will here to tend to be re-bounding via the motion of a Ward-Supplemental-related manner, in the process of going from a condition of moving inward an energy level, into then going into a condition of moving outward an energy level.  Such a re-bounding Fourier-related activity, that is here to work to involve a Ward-Supplemental process, is here to then involve a set of  antiholomorphic Kahler conditions -- which, to an extent, is dependent upon the number of superstrings that work to comprise the overall electron, that is here to act as one respective overall orbifold eigenset, that is present at that given arbitrary electron's energy level and so forth, from within the given arbitrary atom of the said respective case.  Such a set of antiholomorphic Kahler conditions, is to then to rise in so as to form a set of Lagrangian-based Chern-Simons singularities, -- of which will then bear a set of complex roots, depending upon the number of spatial dimensions that the said electron is to be going through, as it is here to be traveling in a back-and-forth manner over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Light Traveling Through A Medium Other Than A Vacuum

Whenever electromagnetic energy is to be traveling through any medium other than a vacuum --   the directly corresponding discrete quanta of electromagnetic energy that are here to be traveling as such, are here to be constantly interacting with other discrete quanta of energy, in a manner that is eminently Yukawa in nature.  As such discrete quanta of electromagnetic energy is to be Gliosis to other discrete quanta of energy, over time -- the directly corresponding scattered quanta of electromagnetic energy is to fidget in such a manner, to where it is here to work to form Lagrangian-based Chern-Simons singularities, -- in such a manner, to where the correlative photons that are here to be scattered, are to travel in the direction of least time.  As such discrete electromagnetic energy is here to be constantly traveling in a general Fourier-related activity, of scattering upon such a general phenomenology over time, -- those eigenstates of discrete energy that are here to be fidgeting, may be said to then be bearing a relatively invariant tense of Chern-Simons singularities, -- since the general activity of a Calabi-related tense of interaction, works to form a general Ward-Cauchy-related condition of then bearing a higher scalar magnitude of a change in the number of derivatives --than the number of spatial dimensions that the said electromagnetic energy is here to be traveling through.
I  will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Chern-Simons Invariants And Orbifolds, Part Two

If such an orbifold eigenset is not of an immediately viable condition of being electromagnetic energy, and if the orbifold eigenset is here to be of a mass-bearing tense, that is here to be in the process of being translocated via a tense of Noether-related flow, -- the individually taken superstrings that are here to work to comprise the said orbifold eigenset, will tend to fidget, per each individually taken iteration of group-related instanton, in one manner or another, in a way that is either  Chern-Simons in a metrical-based manner or Chern-Simons in a Lagrangian-based manner, over each succeeding iteration of discrete time.  This is the tending case, no matter how hermitian the interactive overall orbifold eigenset -- that works to be comprised of by all of the so-mentioned discrete quanta of energy that are here to act as such -- is here to be.  So, a Rham (De Rham) cohomology, that is of an orbifold eigenset -- that is here to be comprised of by many individually taken discrete quanta of energy -- will tend to bear composite superstrings that work to make this up, that will tend to work to bear either metrical and/or Lagrangian-related Chern-Simons Invariant singularities.  Sure, for one thing, just by this, due to the condition of the eminent perturbation of the torsioning of the angular momentum of the holonomic substrate, that is of the so-mentioned mass-bearing superstrings -- such a said perturbation tends to work to change the directoral-related holomorphicity of the composite superstrings, at least by a little, per instanton, and thereby, this alone will tend to perturbate the discrete tensoric field, that is most Yukawa to that Poincare-related field that is Gliosis to the core-field-density of the cohomological activity of the general multiplicit topological stratum -- that works to comprise these given arbitrary respective superstrings, in at least one manner or another to at least some degree of scalar amplitude.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.