Some Definitions

1)  Gravity -- A Chern-Simons translation of Yau-Exact directorals.

2)  Anti Gravity -- A Yau-Exact translation of Chern-Simons directorals.

3)  De Sitter Gravity -- A Harmonic Ricci Scalar metric-gauge translation, that is here to be determined through a Fourier Sequential Series.

4)  Anti-De Sitter Gravity -- An Anharmonic Ricci-Scalar metric-gauge translation, that is here to be determined through a Fourier Sequential Series.

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

The Klein-Gordan Theorem

The Klein-Gordan Theorem is, that -- for every discrete eigenstate of energy permittivity, there is a discrete eigenstate of energy impedance, acting from the reverse-holomorphic direction -- via the light-cone-gauge.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Another Part Of The Puzzle

Now, let us consider another part of the puzzle, in correspondence to the following developing metaphor.  Consider positive and negative spaces scattered together without colliding.  Consider the scattering amplitude of a vibrating oscillation, which allows opposite spaces of chirality to occupy the same general proximal locus, without canceling each other.  Consider this being done by a multiplicit path-loop rectification, -- as may be described of by a multiplicit variation of parameters, that has a Jacobean-Like Wronskian, that is here to be denoted in the said multiplicit variation of parameters of such a metaphorical general case.  Consider the integration done here, to work in so as to be describing an antidifferentiation of what may be the case of either a tightly-knit Fourier  Transformation or of a loosely-bound Laplacian Fourier Transformation. (There is here to be a relatively gradual change in the specific locus of the extrapolated eigenstates of physical states, at the level that is Poincare to the internal reference-frame of these same said extrapolated eigenstates).
Now, here is a broader manner of consideration of a similar gist of the just mentioned concept.  Metaphorically consider all of material phenomena, except for the space-hole, to be an organization of point-commutators and/or ghost-anomalies.  So, material phenomena is not just smooth space, space is what material phenomena is -- except for the space-hole.  The difference between superstrings and freely bound point-commutators in this so-eluded-to metaphor, is that the so-eluded-to strings may be thought of as being he general basis of that material phenomena that most involves what may be extrapolated, by utilizing differential equations that are both exact and linear, -- whereas, the said point commutators in this metaphor, may be thought of as being the general basis of that material phenomena that most involves what may be extrapolated, by utilizing differential equations that are both inexact and non linear.
I will continue with the suspense later!  Sincerely, Sam Roach.

Course 20, Session 13

Electromagnetic energy, including all light, tends to scatter at least to some extent -- if that electromagnetic energy is propagated in an orthogonal nature, upon any given surface of any phenomenon, that the given electromagnetic energy is interfacing upon.  Whenever any electromagnetic energy is orthogonally transferring and propagating through and/or upon a surface or region, the given electromagnetic energy is then to tend to be polarized at least in part, through and/or upon the given surface or region.  However, when electromagnetic energy, in the form of quantized beams of waves, is orthogonal as a field -- to any plain kinetic energy that exists as a field, then, the said electromagnetic energy will tend to be absorbed as opposed to being scattered.  If the given electromagnetic energy is not completely polarized, and is thus scattered to some degree, then the electromagnetic energy that is here to be striking a tense of plain kinetic energy in a manner by which it is scattered, must then switch its genus of topology, right after the light is to scatter upon the surface of the given said plain energy.  That would mean, that the electromagnetic energy that is scattered here, would change temporarily, from initially having a Yang-Mills topology to then working to bear a Kaluza-Klein topology.  This here would mean that the Clifford Algebra here, would then be converting from working to bear a euclidean and hermitian geometry, into then working to bear a euler and Dirac geometry, for the time being.  Once that the given electromagnetic energy is scattered, the Gaussian of the superstringular part of the said electromagnetic energy, is to switch back in its light-cone-gauge orientation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Positive And Negative Charges And Cohomology

An orbifold eigenset that is to rapidly cycle in a relative manner, from going back-and-forth from generating cohomology-related eigenstates to degenerating cohomology-related eigenstates, and so on, will tend to both work to bear a negative charge, be of a relatively small size, and will also tend to be brought into a motion that is of a relatively high velocity, -- whereas, an orbifold eigenset that is, instead, to gradually cycle in a relative manner, from going back-and-forth from generating cohomology-related eigenstates to degenerating cohomology-related eigenstates, and so on, -- will tend to both work to bear a positive charge, be of a relatively larger size, and will also tend to be brought into a motion that is of a relatively low velocity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David 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.

Interim Before Session 13 Of Course 20

Let us initially consider a superstring of discrete energy permittivity, that behaves as a single unique orbifold eigenset -- that is differentiating here in a Fourier-based manner, in so as to travel through a mean Lagrangian-based path -- as potentially being of a Yau-Exact discrete quantum of mass-bearing energy.  Let us say that -- if the so-stated superstring of this case were to change in two derivatives, as the said superstring is here in the process of traveling along a two-spatial dimensional Minkowski-based Hamiltonian operand, to where the thus formed genus of the singularity, that would thus be formed at the specific locus where the so-eluded-to change in concavity is here to happen -- would then be of a hermitian-related singularity, -- in as long as the cohomological-based tracing of the correlative integration of the ghost-based indices, that would thus be formed, were of a purely Real Reimmanian-related nature, to where there would here be no Nijenhuis nor Doubolt-based spurs to be considered in this given arbitrary case, in neither a metric nor in a Lagrangian-based manner.  Next, let us consider here, the same initially stated superstring of discrete energy permittivity, that is acting as a single given arbitrary orbifold eigenset -- that is moving via a mean path -- through a two-dimensional unitary Lagrangian-based path, that instead, is to change all of the sudden in four derivatives, as it is still moving through a two-spatial-dimensional Hamiltonian operand, immediately prior to the so-eluded-to perturbative kinematic activity -- that would then act in so as to effect the Kahler condition of the ghost-based pattern, that would here be directly affiliated with the cohomology-based mappable-tracing, that is of the so-eluded-to bosonic superstring, of which would here work to produce the conditions of a Lagrangian-based Chern-Simons singularity, that would be of a correlative Fourier-based Hamiltonian operator, that would here potentially be of some genus of a Calabi-Yau related manifold, that would be in the process of being propagated as a Noether-based set of eigenindices, that would here occasionally work to bear an influence upon a relatively loosely knit tense of a Majorana-Weyl-Invariant-Mode, immediately prior to the so-eluded-to Chern-Simons-related perturbation.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

Course 20 Session 14

There are more interactions between electromagnetic energy and its surroundings, than just Calabi-Yau and Calabi-Wilson-Gordan interactions.  In other words, light, and for that "matter," any form of electromagnetic energy, does not necessarily just scatter upon matter, and, light and any form of electromagnetic energy, does not necessarily just scatter upon plain kinetic energy too.  Light, or as well, any form of electromagnetic energy -- may also at times, scatter upon other plain electromagnetic energy itself.  So, an electromagnetic beam, or, a set of quantized electromagnetic beams, may occasionally -- scatter upon another electromagnetic beam, or, another set of electromagnetic beams. When light or any other form of electromagnetic energy, scatters upon any set of one or more electromagnetic beams -- the genus of the interactions that will then ensue to happen here, -- may then be described of here in my string theory model, as being a Calabi-Calabi interaction.  A Calabi-Calabi- interaction -- is to often be happening, under the correlative Ward-Cauchy-based conditions that are here to directly be corresponding, when as set of electromagnetic energy is to strike an ulterior set of electromagnetic energy, as as Fourier-related Yukawa transference, that may be thought of as happening at an acute angle -- at a level that is Poincare to the external shell, that is of the homological surface that is of the so-eluded-to Gliosis-related interaction.  However, if, under the correlative Ward-Cauchy-based conditions,  there is here to be, instead, a tense of an obtuse angle --  that is to be transferred at the point in duration, in which the two different said sets of electromagnetic beams are to be translated upon each other in a Gliosi-related manner, -- in so to work to form the proximal local conditions of norm-based conditions, -- that are here to be interdependently correlative, between the two given arbitrary said sets of electromagnetic energy, that have here to have struck each other -- then, the two different said sets of electromagnetic energy will consequently move in so as to quantize among each other instead.  I will continue with the suspense later! To Be Continued!  Sincerely, Sam Roach.

Schwinger-Indices And Centralized Knotting

Gauge-Bosons act, in so as to work to "pluck" their directly corresponding second-order light-cone-gauge eigenstates like a harp -- in so as to work to form those multiplicit Schwinger-Indices, -- that act along the Rarita Structure, in so as to work to help in the allowance of the four different general classifications of the general attribute of "force."  When such said Schwinger-Indices are to come together, in so as to work to form waves -- of which are here to move in such a manner, in so as to propagate in a way that is both transversal and perpendicular --  to where this is to form such waves that may vary here from bearing a wavelength that may be between 5*10^(-22)Meters in length to 4*10^(-18)Meters in length, -- this will then work to tend to form the basic increments of the gravitational force.  If however, such said Schwinger-Indices are to instead, to work in so as to help to strengthen the multiplicit eigenstates of the centralized knotting of the Rarita Structure, -- then, such a general manner of operation, is here to work to tend to help in the fortification of the strong force.  Furthermore, -- the general interaction that is to be between photons and the multiplicit light-cone-gauge, is to work to influence both the ensuing Schwinger-Indices that are thence formed, as well as working to influence those correlative Schwinger-Indices that are here to be proximal local, to such an earlier inferred general genus of operation -- will tend to work to help at forming the electrostatic force.  Consequently -- the general activity of such a so-eluded-to genus of Schwinger-Indices, -- to act in so as to work to weaken the knotting structure of the multiplicit centralized knotting of the Rarita Structure, -- will then work to help in potentially allowing to form those conditions, in which the weak force may then work to become eminent.
 I will continue the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Calabi-Interactions, Session 12

As an initially obvious statement -- electromagnetic energy not only scatters upon matter -- yet, it may also scatter upon plain kinetic energy as well.  The process of electromagnetic energy scattering upon plain kinetic energy, may be thought of as being a Calabi-Wilson-Gordan interaction.  Whenever light, or, whenever any electromagnetic energy if you will, is to be propagated through time and space, -- it is comprised of waves that are here to exist as a compilation of tiny discrete particles, that are known of as being called photons.  An individual photon has, during any given arbitrary iteration of group-related instanton, located at a positioning that is coming from the said photons reverse-holomorphic side -- the existence of a Ward-Cauchy-related phenomenology, that may be described of here as being a Fadeev-Popov-Trace eigenstate.  Such a said Fadeev-Popov-Trace eigenstate is here to be connected to the said discrete quantum of energy permittivity (the particle nature of the said "photons"), by manner of the so-eluded-to discrete quantum of energy -- by what may here be described of as a discrete first-order light-cone-gauge eigenstate.  The superstring of such a photon is here to behave as being the discrete particle-based quantum of energy permittivity; the counter string of such a photon is here to behave as being the discrete wave-based quantum of energy permittivity; the Fadeev-Popov-Trace eigenstate of such a photon is here to behave as being the discrete particle-based quantum of energy impedance;  And the first-order light-cone-gauge eigenstate of such a photon is here to behave as being the discrete wave-based quantum of energy impedance.  When one is here to to in a Laplacian-based manner -- from the given arbitrary Fadeev-Popov-Trace eigenstate of a respective case to the counter string of the same respective given arbitrary counter string of such a said case, -- then, one is here to be going in a Laplacian-based manner, in the relative forward-holomorphic direction.  With all of that in mind -- when a beam of electromagnetic energy is here to strike any given arbitrary field of plain kinetic energy, the so-eluded-to radiation may either become fully absorbed in the respective said entered field, or the radiation may be partially absorbed and partially scattered by the respective said entered field, or, the radiation may then become fully scattered by the respective said entered field.  This will depend upon both the angle and the relative delineation of the said strike of the said radiation upon the said field of plain kinetic energy. 
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Part Of What May Happen To Work To Cause Tachyonic Motion

When a superstring of discrete energy permittivity is to be both vibrating anharmonically in an odd number of spatial dimensions in the relative forward-holomorphic direction, at the duration that is right before instanton, and if, as well, the here mentioned superstring of discrete energy permittivity is to be vibrating harmonically in an odd number of spatial dimensions in the relative reverse-holomorphic direction, during the ensuing proximal local Regge Action, then, such a so-mentioned superstring of discrete energy permittivity, will then ensue to become of a tachyonic manner.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Dimensional Compactification And Stringular Settling

The general activity of that particular genus of activity that is to happen, as a superstring and its correlative counter string of discrete energy permittivity, is to go into a transient Ward-Cauchy-state of dimensional compactification, as such a quantum of discrete energy and its counter part is about to go into its ensuing iteration of group-related instanton -- tends to work to help the said superstring and its counter part to then to be able to settle into the said ensuing iteration of group-related instanton.  Consequently -- the general activity of that particular genus of activity that is to happen, as a superstring and its correlative counter string of discrete energy permittivity, is to go into a transient Ward-Cauchy-state of dimensional decompactification, as such a quantum of discrete energy and its counter part is about to go into its ensuing iteration of the Regge Action -- tends to work to help the said superstring and its counter part to then able to become prepared to go into the so-eluded-to iteration of the generally unnoticed duration of Ultimon Flow.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Partition-Based Discrepancies And Orientation

When a superstring of discrete energy permittivity is here to work, to bear a tense of superstringular orientation, during BRST -- the directly corresponding partition-based discrepancies that are of the correlative superstring of discrete energy permittivity, are here to be completely assymetrical in delineation towards its correlative counter string -- over the course of the self-same iteration of the said increment of BRST.  This may then be said to bear a condition, of such a Ward-Cauchy-related field, that is here to be in-between the said superstrings and its correlative counter string -- to be of a homeomorphic nature.  However -- if the Beti number that is here to be directly corresponding to a discrete quantum of energy -- from right before an interation of BRST, is to be of an odd number, then, both the directly corresponding superstring and its correlative counter string, will, in an individually taken manner -- at such a so-eluded-to point in duration, that is here to be just before an iteration of group-related instanton, to act in so that it will be vibrating annharmonically in an odd number of spatial dimensions in a holomorphic manner, that is here respective to the same number of spatial dimensions that such a superstring and its correlative counter string, will both individually contract by, when this is taken at the said general instance, that is here to be at the moment just before the said iteration of group-related instanton.  (BRST being at the beginning of the said instanton.)  When the just mentioned general tendency of vibration, is to happen to a respective superstring and its correlative counter string, then, the earlier said tendency of a homeomorphic field -- is to not to be able to happen.  This will then tend to work to cause such a so-eluded-to discrete quantum of energy, to not to be orientable during the here correlative iteration of the Beti Action.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Orbifold Eigensets And Orientable Manifolds

Whenever an orbifold eigenset is conditioned to be of an unorientable nature -- this will then be of such a Ward-Cauchy-related condition, to where -- those discrete energy quanta that are to work here to act, in so as to comprise the said orbifold eigenset, are to be, as well, of an unorientable nature.  Yet, consequently, whenever the superstrings of discrete energy permittivity -- that are to here to be of a directly corresponding orbifold eigenset -- are to be conditioned to be of an orientable nature, then, the correlative respective orbifold eigenset as a whole, will, as well, act in so as to be of an orientable nature.  Gauge-Bosons will always tend to work to display, the same number of spatial dimensions, as whatever the number of spatial dimensions that the directly corresponding core field that the multiplicit affiliated superstring of discrete energy permittivity will then tend to display.  Consequently -- since the core field of any one given respective superstring of discrete energy permittivity, is to tend to have one more spatial dimension than such a said string, -- not only is an orbifold eigenset to tend to bear just as many spatial dimensions as all of the individually taken superstrings of discrete energy permittivity, that are here to work to comprise the said eigenset, -- yet also, -- all of the gauge-bosons that are here to be most directly affiliated with such an orbifold eigenset, will tend to bear one more spatial dimension than the orbifold eigenset will tend to have, at an internal reference-frame.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Compact Manifolds

If an orbifold eigenset is to be of a cotangent bundle of phenomenology, that is here to be of a given arbitrary number of spatial dimensions, then, such an orbifold eigenset that is consequently to be moving via the general manner of Noether Flow, is said to work to maintain -- during the course of the correlative evenly-gauged Hamiltonian eigenmetric, in which it is here to be of a compact nature -- then, the  general Ward-Cauchy-related condition, of remaining as a manifold of a discrete overall quanta of energy, that is here to be of one specific number of spatial dimensions, will then be at what is here to be at the vantage point of a relatively respective internal reference-frame.  This will then mean, -- that if an orbifold eigenset is to be of what is to here to be of a compact nature, -- that, as this is to be in the process of being the general case -- that, for each of such so-eluded-to iterations of group-related instantons, that the Beti number that is here to be of the individually taken superstrings of discrete energy permittivity, that are here to work to help at comprising the earlier mentioned orbifold eigenset -- as it is to be just about to enter the Ward-Cauchy-related process of group-related instanton, is to be of the same absolute value of such a correlative Beti number, that is here to be of the individually taken superstrings of discrete energy permittivity that are here to work to help at comprising the earlier mentioned orbifold eigenset -- as it is to be entering the ensuing general gauge-action of the Regge Action.  This will then mean -- that the Beti number for all of the individually taken superstrings that are here to work to comprise the said orbifold eigenset, at a vantage-point of such a respective eigenset, as it is to be just about ready to enter its correlative iteration of group-related instanton, is to be of an even positive integer (for compactification), as well as the Ward-Cauchy-condition, that all of the individually taken superstrings that are here to work to comprise the said orbifold eigenset, at a vantage-point of such a respective eigenset -- as it is to be working to enter its ensuing iteration of the Regge Action, is to be of an even negative integer (for decompactification) (to where the earlier mentioned positive integer is to bear the same scalar matgnitude from zero as the earlier mentioned negative integer), to where such said superstrings of such a given respective case, are to here to not vary in the number of spatial dimensions that these are here to have, over the correlative so-eluded-to sequential series of the directly corresponding iterations of BRST.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Anharmomic Vibration And Stringular Compactification

When an orbifold eigenset is to compactify by one given arbitrary number of spatial dimensions, then, all of the superstrings that are of the same one respective given arbitrary orbifold eigenset of such a case, will compactify by the same number of spatial dimensions.  So, all of the individually taken superstrings of discrete energy permittivity, that are here to work to comprise one correlative given respective orbifold eigenset -- will be vibrating in an anharmonic manner in a holomorphic manner, in the same number of spatial dimensions, -- at that general point in duration, that is here to be at the general moment that is to be taken right before the start of the correlative beginning of one specific iteration of group-related instanton.  So, if one individually taken superstring of discrete energy permittivity, is to be orientable during a correlative iteration of the Beti Action, -- then, all of the individually taken superstrings of discrete energy permittivity that are of the same orbifold eigenset, will be orientable during the self-same correlative iteration of the Beti Action.  Consequently -- if one individually taken superstring of discrete energy permittivity, is to be unorientable during a correlative iteration of the Beti Action, -- then, all of the individually taken superstrings of discrete energy permittivity that are of the same orbifold eigenset, will be unorientable during the self-same correlative iteration of the Beti Action.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Superstringular Distortion Right Before BRST

If the distortion that is here to happen to any one given arbitrary superstring of discrete energy permittivity, right before such a said string is to go into its next ensuing iteration of instanton, is to be of a harmonic nature -- then, such a said given arbitrary respective superstring of discrete energy permitttivity, shall, at the said general point in duration that is to here to be right before the so-eluded-to start of its ensuing iteration of instanton, to work to bear an anharmonic vibrational oscillation in the relatively forward-holomorphic direction in an even number of spatial dimensions, at the said earlier mentioned general point in duration.  The said string is to then to compactify in an even number of spatial dimensions at the general point that is right before instanton in this given respective case.  This will then work to helping to allow the said superstring to be orientable during the ensuing Beti Action, -- since this will then work to help such a said superstring to bear a homeomorphic field, that is here to be accounted for, in-between the directly corresponding string and its correlative counter string.  However -- if the distortion that is here to happen to any one given arbitrary superstring of discrete energy permittivty, right before such a said string is to go into its next ensuing iteration of instanton, is to be of an anharmonic nature -- then, such a said given arbitrary respective superstring of discrete energy permittivity shall, at the said general point in duration that is to here to be right before the so-eluded-to start of its ensuing iteration of instanton, to work to bear anharmonic vibrational oscillation in the relatively forward-holomorphic direction in an odd number of spatial dimensions at the said earlier mentioned general point in duration.  The said string is to then to compactify in an odd number of spatial dimensions at the said general point, that is right before instanton in this given respective case.  This will then work to help to cause the said superstring to be unorientable during the ensuing Beti Action, -- since this will then work to cause such a said superstring to Not to be able to bear a homeomorphic field that would here to be accounted for, in-between the directly corresponding string and its counter string.  I will continue with the suspense later!  To Be Continued! 
Sincerely, Samuel David Roach.

Some Basic Information As To The Slater Equation

The main purpose as to what the Slater Equation is utilized for, in the microscopic realm -- is to show what the mean Lagrangian-based path is, that may be translated -- through a correlative Hamiltonian operand.
I will continue with the suspense later!  To Be Continued!  Sincerely Samuel David Roach.

Orbifolds And Abelian Nature

Let us initially consider an orbifold eigenset.  All of the discrete quanta of energy that work to help comprise the just mentioned orbifold eigenset, will work to conform to the same tense of a genus of a light-cone-gauge topology.  So, if one were to have an orbifold eigenset that is here of a Kaluza-Klien light-cone-gauge topology, then, all of those discrete quanta of energy that are here to work to comprise the said orbifold eigenset -- will as well work to bear a Kaluza-Klein light-cone-gauge topology.  Furthermore, -- if one were to have an orbifold eigenset that is here of a Yang-Mills light-cone-gauge topology, then, all of those discrete quanta of energy that are here to work to comprise the said orbifold eigenset -- will then work to bear a Yang-Mills light-cone-gauge topology, and for the same apparent reason.  A Kaluza-Klein light-cone-gauge topology is said to be abelian, whereas, a Yang-Mills light-cone-gauge topology is said to be non abelian.  I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

Schwinger-Indices And Mass

Let us initially say that one is here to be considering a mass-bearing phenomenon -- that is here to be comprised of many orbifold eigensets, that are to come together, in so as to work to form one complete entity.  Each of the discrete quanta of energy, that are here to work to help in the process of comprising the so-eluded-to relatively macroscopic phenomenology of mass -- are to be emitting a propagation-related set of Schwinger-Indices, that are to come together in so as to work to form gravitational waves.  As such said gravitational waves are to here to be propagating outward -- in a manner that is both perpendicular and transversal over time, -- such a said propagation of gravitational waves, in turn, is, in the process of such a set of so-eluded-to vibration-related oscillations, that are to here to be tugging relatively outward, are to work to help in the "tightening" of certain eigenstates, that are of the centralized knotting of the Rarita Structure.  Such a said process of a tightening of those so-stated eigenstates, that act as nodes along the Rarita Structure, is, in turn, to help in the process of working to form the needed attributes of the strong force.  This should make things clearer to the reader.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Schwinger-Indices And The Strong Force

The propagation of Those Schwinger-Indices over time -- that are here to come together, in so as to work at forming gravitational waves -- works to help at tightening the region at which there are those eigenstates, that are here to be of the centralized knotting of the Rarita Structure.  Such a said "tightening" of those eigenstates, that are here of the centralized knotting of the Rarita Structure, consequently works to help at forming mesons such as gluons.  This then works to mean, that the Propagation of gravitational waves, works to help at forming those essential attributes, that are here to be needed, in so as to help at forming the strong force.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

i*PI(del) Action And Magnetism

The lower that the rate is of the i*PI(del) action -- at internal reference-frame -- of any one given arbitrary relative proximal local tense of a Ward-Cauchy-related region, at which a given arbitrary orbifold eigenset is to be over time, the higher that the relative tense of the directly corresponding reverse-fractal of magnetism will tend to be at a level that is less microscopic.  Likewise, -- the higher that the rate is of the i*PI(del) action -- at an internal reference-frame -- of any one given arbitrary relative proximal local tense of a Ward-Cauchy-related region, at which a given arbitrary orbifold eigenset is to be over time, the lower that the relative tense of the directly corresponding reverse-fractal of magnetism will tend to be at a level that is less microscopic.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Frequency And General Tense Of Majorana-Weyl-Invariant-Mode

The higher that the general tense of the frequency of the vibration of an orbifold eigenset is to be -- when this is to be taken as to the frequency, that is of the rate at which the said orbifold egienset is to be oscillating at at its internal reference-frame -- this will then tend to work to help at causing a lower tense of a Majorana-Weyl-Invariant-Mode, than an ulterior orbifold eigenset, that is here to be vibrating at a lower frequency.  If any one given arbitrary orbifold eigenset is to, instead, to bear a higher tense of a correlative Majorana-Weyl-Invariant-Mode -- over an evenly-gauged Hamiltonian eigenmetric -- then, it will then tend to work to bear a tense that is of its composite strings, -- that will, in such a case, tend to be of a lower frequency of their correlative vibrational oscillations, -- to where such a so-eluded-to set of discrete energy that is to perform one specific function over time (of which is a general description of an orbifold eigenset), will then tend to bear more of a resonant vibration, as such a set of superstrings that are here to work to help at comprising the said orbifold eigenset, will, at a reverse-fractal tense, tend to bear a higher tense of magnetism, than a respective set of orbifold eigensets will tend to have, -- at a reverse-fractal tense from the Ward-Cauchy bounds of such a here considered orbifold eigenset.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel  David Roach.