Metaphorical Thoughts

 Let’s say, that one were to figuratively liken, the multiplicity of space time fabric, to the multiplicity of language. One could then metaphorically consider: the nouns to be likened to the Hamiltonians, the verbs to be likened to the Lagrangians, the adjectives to be somewhat likened to the metric gauge, the adverbs to be somewhat likened to the heuristic gauge, and the prepositions to be likened to the re-calibration of Chern-Simons singularities. 

I will certainly continue with the suspense Later! ‘Till then, I hope you are having a good day, and make today the most phenomenal day of your life! Sincerely, Sam Roach (1989).

String theory is the metaphorical language of energy, and Fourier-Analysis is the metaphorical language of waves. Energy is both wave and particle based. This gives one an idea, as to Why Fourier-Analysis is so crucial to string theory. 

Entropy is energy of heat transfer per Kelvin Mole. Entropy that is conveyed in a De Rham manner, often tends to bear a benevolent physical nature. Whereas; Entropy that is conveyed in a Dolbeault manner, often tends to bear a malignant physical nature. Although at least some entropy is necessary, for various changes in physical states to occur, it is my theory, that even though it goes against the second “law” of thermodynamics, that it is possible, to be able to viably decrease, at least some of the scalar effectual presence, of the multiplicity, of malignant entropy. 

Harmonically propagated sound, often tends to work to bear a tense of consonant vibration. Whereas; Anharmonic associated propagated sound, often tends to bear a tense of dissonant vibration. Consonant vibration may often tend to facilitate, the generation of resonant pulsation. Whereas; Dissonant vibration may often tend to facilitate, the degeneration of resonant pulsation. One may think of resonant pulsation, in a way, as being the physical manifestation, of the inverse of isotropically stable thought frequency. 

Whenever a physical phenomenon is kinematically propagated and/or transferred through space (over a duration of time), this will inevitably work to involve a system of waves. Therefore; Whenever a time-related physical occurrence is to take place, such an occurrence will inextricably tend to work to involve, at least some sort of Fourier-Related System, since waves are thus involved. 

When one is dealing with a system of waves, that is taking place in Less than one discrete increment of time, one may, perchance, call this, a Laplacian-Related "activity," as taken from within the scope of a tightly-knit Fourier-Related situation. Remember: Fourier-Related Analysis, is the language of waves. 

Consider the following: Take a theoretical snapshot of a wave-based delineation, of a given arbitrary proscribed system of waves, over the course of one Planck-Related instance. Next; Take a theoretical snapshot of the wave-based delineation of the same system of waves, yet over the ensuing course of the proceeding Planck-Related instance. Keep going as such. Now; recursively display the respective sequential series, of the integrative set, that is of such theoretical snapshots, in the proscribed order that these were taken. This will give one a viable indication, as to the wave-related progression, if taken in the insinuated piecewise continuous manner eluded to, to where, this general procedure, will work to facilitate a knowledge, as to the eminently corroborative, given arbitrary Fourier-Related-Progression, that is here to be, of such a particular genus of a case scenario. When given in lieu of its Lagrangian-Based Drive, this will tend to work to refine, such a facilitation, as to understanding how such a wave-based system enfolds, to where the metaphorical artifacts of knowing how such a system is to proceed, is thus enhanced. 

Here is a procedural hint, in so as to facilitate being able to determine Chern-Simons Invariant gauge-actions, in general, for the arbitrary genus of case scenario, involving co-tangent bundle R3.:

1) Consider the trace depiction of the motion, that is of the eminently corroborative Hamiltonian Topological Manifold, being mathematically worked with here, as taken at a snapshot of its delineation, in terms of the mathematical physics description, that is here to describe the way that the minimal surface, that is implicitly mentioned here is to be mapped out — as a generic pattern of mappable oscillation.

2) Consider the given arbitrary, eminently involved mathematical physics expression, of kinematically propagational-related import, that is most relevant to the suitings, of such a respectively proscribed case scenario. 

3) Take both the first order integral, and, the second order integral, of the just mentioned expression of kinematically propagational-related import, in respect to a durational parameter of variable. 

4) Take the last three implicit values of kinematically propagational-related import, and add them together. 

5) Consider the just mentioned summation, as one whole group. 

6) Consider the directional attributes, that the gauge-action being considered, is inextricably to be taken in. 

7) Multiply the initial implicitly mentioned vector trace, by the latter mentioned grouping. 

8) Next; Multiply this whole thing, by 2/3 — since the reductional minimal surface is heuristically in two spatial dimensions, and the gauge-action is of co-tangent bundle R3. 

9) Divide the entirety of what has been described so far, at this point, by 4*PI. 

10) The result of this math, in many general cases, will facilitate an endeavor, to determine the vector value, of certain proscribed cases, in terms of finding the desirable Chern-Simons Invariant Gauge-Action, of what this is to be eminently corroborative to happen to be in the process of finding out, in lieu of acting to better understand that metaphorical grip hold of wave tug, whose alterations spew into charge and or entropy. 

In a metaphorical nutshell: The i*PI(Del)Action, amounts to being — Unitary heuristic-gauged magnetic potential. 

Whenever individually taken Chern-Simons Invariant gauge-actions are re-calibrated, unitary heuristic-gauged magnetic potential is generated. When such a respectively indicated potential is to couple with a discrete quantum of angular frequency, in at least a fairly hermitian manner, this will generally tend to form charge.,Yet; If, instead, such a respectively indicated potential is to couple with a discrete quantum of angular momentum, again, in at least a fairly hermitian manner, this will generally tend to form entropy. 

Here’s a nifty metaphor I recently thought of: The Higgs Field in physics is to mass, what the Ribosomes in biology are to protein!

The Majorana-Weyl-Invariant Field in physics is to mass, what the Golgi Apparatus in biology is to protein. 

Thought Waves That Often Tend To Be Most Succinctly Incurred

 Thought waves of an isotropic nature, that are of both a relatively small wavelength, while also acting as respective individually taken solitons, often tend to be more capable, of being able to most succinctly incur upon the neurons of the subconscious mind of the brain of a biological entity, than other genre of thought waves do. I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH.

As To The Conveyance Of Thought Waves

 The More hermitian (the Less Spurious), that a given arbitrary set of thought waves is to be delineated as, over the course of a given arbitrary duration of time, -- the more harmonic that the conveyance of such thought waves, will consequently result, in tending to be. Therefore; The Less hermitian (The More Spurious) that a given arbitrary set of thought waves is to be delineated as, over the course of a given arbitrary duration of time, -- the less harmonic that the conveyance of such thought waves, will consequently result in tending to be. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

More As To Cohesive Set Of Norm-State-Projections

 Again; At a flush delineation of perspective, that is here to be taken, at a vantage-point that is immediately external to the Poincare level, of the Laplacian-Based mappable-tracing, of each of the following of what is soon to de described, I have perceived that the following may be true, about the individually taken directly associated cohesive set of norm-state-projections:

When one is to  have a given arbitrary cohesive set of Campbell norm-state-projections, that are here to work to be bear a covariant Yukawa inter-relationship amongst themselves, -- there is a relatively high probability, that the appearance of the mappable-tracing, of the intersecting wave-like tense, that one will consequently tend to observe, will often tend to bear a morphology, that is consequently of a resultant set of intersecting Inverted sinusoidal wave-like phenomenology. Furthermore; When one is to have a given arbitrary cohesive set of Campbell-Hausendorf norm-state-projections, that are here to work to bear a covariant Yukawa inter-relationship, -- there is a relatively high probability, that the appearance of the mappable-tracing, of the intersecting wave-like tense, that one will consequently tend to observe, will often tend to bear a morphology, that is consequently of a resultant set of intersecting perturbative sinusoidal/perturbative Inverted sinusoidal wave-like phenomenology. Sincerely, SAMUEL ROACH. 

Cohesive Set Of Norm-State-Projections -- Tense Of Wave-Like Intersection

 At a flush delineation of perspective, that is here to be taken at a vantage-point that is immediately external to the Poincare level, of the Laplacian-Based mappable-tracing, of each of the following soon to be described, individually taken directly associated cohesive set of norm-state-projections: 

When one is to have a given arbitrary cohesive set of Hausendorf norm-state-projections, that are here to work to bear a covariant Yukawa inter-relationship -- one will consequently tend to have here, a greater probability, of having the resultant mappable-tracing, of a set of intersecting sinusoidal wave-like phenomenology, Than a resultant mappable-tracing of a set of intersecting square wave-like phenomenology.  Furthermore; when one is to have a given arbitrary cohesive set of zero-norm-state-projections, that are here to work to bear a covariant Yukawa inter-relationship -- one will consequently tend to have here, a greater probability, of having the resultant mappable-tracing, of a set of intersecting square wave-like phenomenology, Than the resultant mappable-tracing of a set of intersecting sinusoidal wave-like phenomenology. TO BE CONTINUED!  Sincerely, SAMUEL DAVID ROACH. (1989).

Anti Gravity/Gravity -- Wave-Tug

 The general phenomenology of anti gravitational waves, tends to have the ability of working to help, in the enhancement of the potential capacity of the wave-tug, of those kinematic angular momentum-related eigenstates, that are here to help in working to form the general basis, of the physical directional drive, in the multiplicity of the motion of physical phenomenology, over a directly corresponding period of time; whereas, -- the general phenomenology of gravitational waves, tends to work Against the general process of working to help, in the enhancement of the potential capacity of the wave-tug, of those kinematic angular momentum-related eigenstates, that are here to help in working to form the general basis, of the physical directional drive, in the multiplicity of the motion of physical phenomenology, over a directly corresponding period of time. I will continue with the suspense later! Sincerely, SAMUEL ROACH. (1989). 

Interface Of Waves, And Radio Signal Harmonics

 The Gliosis-related application of a harmonic interface, as taken between thought waves and gravitational waves, upon any given arbitrary radio signal, -- tends to help to work to harmonize the mentioned general radio signal, whereas; the Gliosis-related application of an anharmonic interface, as taken between thought waves and gravitational waves, upon any given arbitrary radio signal, -- tends to help to work to distort the mentioned general radio signal. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (1989).

Harmonic/Anharmonic Mode

When thought waves are to work to bear a harmonic interface with gravitational waves, this will tend to bear the capacity, of working at helping to form a harmonic oscillation-based mode -- upon those correlative Fadeev-Popov-Trace eigenstates, that are proximal local to the general field, at which such an earlier inferred interface, is here to be happening. Furthermore; when thought waves are to work to bear an anharmonic interface with gravitational waves, this will tend to bear the capacity, of working at helping to form an anharmonic oscillation-based mode -- upon those correlative Fadeev-Popov-Trace eigenstates, that are proximal local to the general field, at which such an earlier inferred interface, is here to be happening. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (1989).

Thought Waves And Less Impedance-Related Constriction

 Since the physical entity of thought waves, are to tend to be propagated in a manner, that is to be both simultaneously transversal and supplemental, via the vantage-point of a central coni-point  (instead of being propagated in a manner, that is to be both simultaneously transversal and perpendicular, via the vantage-point of a central coni-point, such as with the ulterior physical entity of gravitational waves) -- as well as there also being the general physical condition, that thought waves tend to work to bear a greater variety of potential wavelengths than gravity waves do, the general physical entity of thought waves, tends to be less inhibited, by the constriction of the physical impedance of the entity of pressurized vacuum, than the general entity of gravity waves are. Thereby, by this just mentioned general condition alone;  thought waves tend to work to bear a greater potential of influence upon their physical environment, than the phenomenology of gravity waves do. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Thought Waves; Both Of Low Wavelength And Of High Frequency

 Thought waves, that are here to be of the nature of having both a relatively low wavelength and a relatively high frequency, -- will consequently tend to work to bear a greater attribute of exhibiting a soliton-like nature, than ulterior types of thought waves, -- that are here to otherwise work to bear both a relatively greater wavelength, and/or working to bear a relatively lower frequency. To Be Continued! SAM ROACH.

Abelian Nature Of Thought Waves

 Let us consider here, that one were to have two different thought waves.  Each of such said thought waves, is here to be in the process of transmitting the same frequency, -- as well as the general condition, being here, that both of such said thought waves, are otherwise to be of basically the same nature, except that one of these two different mentioned thought waves, is here to bear a smaller scalar amplitude of wavelength, than the other of these two different said thought waves. That thought wave of the two, that is here to be of a smaller scalar amplitude of wavelength, will tend to work to bear a greater scalar attribute of an abelian nature -- than the other of the two different said thought waves.  SAMUEL DAVID ROACH.

Electromagnetic Radiation/Thought Waves, Direction Of Least Time

 Electromagnetic radiation tends to move into the direction of least time. I believe that thought waves are capable of making a Yukawa Coupling with waves of electromagnetic radiation. So; when thought waves make a Yukawa Coupling with electromagnetic radiation, these thought waves, as well, will consequently tend to be drawn into the direction of  least time. To Be Continued! Sincerely, Samuel David Roach.

Mini-Stringular Segmentation And Second-Order Point Particles

In regards to my particular model of string theory, what works to form the intrinsic binding of the multiplicit homotopic inter-connections of Ward-Cauchy-based fields, that are here to exist in the substringular, is the the kinematic presence of what I term of as being "mini-stringular segmentation."  Mini-Stringular segmentation, is what tends to bind the vast array of substringular fields together, -- and this is comprised of here by what I term of as being tiny "beads" of second-order point particles, that are here to be held together by what I term of as being the kinematic presence of "sub-mini-string."  These just mentioned second-order point particles may be thought of as being balled-up third-order point particles, that are here to tend to be subtended, in a relatively invariant manner at an internal reference-frame,  from within the general Ward-Neumman bounds of these said second-order point particles.  Consequently; as the kinematic disturbances in space, that are of the wave-related vibrational oscillations of mini-stringular segmentation, -- is to become codifferentiable with its environment in a kinematic manner, to where this is thence to work to form the general tense of that multiplicit perturbation in time and space, that is here to work to allow for the general covariance of the wave-based interaction of such inferred superstringular fields, those second-order point particles are consequently to tend to bear a relative tense of conformal invariance at an internal reference-frame, even as the so-eluded-to external reference-frame that is here to be of the mini-stringular segmentation itself, is here to bear a relative tense of a continual covariant wave-related perturbation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Sinusoidal Holomorphic Tendency Squared

Let's take into consideration here, an orbifold eigenset -- that is here to heuristically be initially traveling in the relative holomorphic direction, in a sinusoidal manner.  Let's next say, -- that one is here -- in this given arbitrary case -- to call the relative holomorphic direction, to be traveling "straight ahead," to where this said eigenset is to then to be traveling "into the page" (metaphorically), as a cross-product-related tendency, that is here to be initially explicitly exhibited.  Next, -- let's say that there is then to be a spontaneous Yukawa Coupling, that is here to be imparted upon the so-stated orbifold eigenset, -- that is here to act upon the sinusoidal oscillation-related tendency of this eigenset, in so as to square the oscillation-based nature of the flow of that sinusoidal wave pattern, -- that this said orbifold eigenset had initially been exhibiting -- at the onset of its translation along the initially inferred relative forward-holomorphic direction, over the course of a relatively transient sequential series of group-related instantons (that may be considered here, to be occurring, over an evenly-gauged Hamiltonian eigenmetric.)  Let's next consider here, arbitrarily, that the forward-holomorphic direction in this particular case, is to be described of as being in the "i" direction;  The reverse-holomorphic direction in this particular case, is here to be described of as being in the "-i" direction;  The forward-holomorphic direction (again, in this case, this is in the "straight-forward" direction), is to be in the "positive x" direction;  The reverse-holomorphic direction (in this  case, this is in the direction that is coming "towards you"), is to be in the "negative x" direction;  The norm-to-forward-holomorphic direction (in this case, this is to the relative "top"), is to be in the relative "y" direction;  And the norm-to-reverse-holomorphic direction ( in this case, this is to be at the relative "bottom"), to where this is to be in the relative "-y" direction.)  Let's next consider, that the Nijenhuis-to-forward-holomorphic direction is here to be of the relative "z" direction (this is to be at the relative "left") ; While the Nijenhis-to-reverse-holomorphic direction is here to be of the relative "-z" direction (this is to be at the relative "right")  .Consequently, the initial heuristic sinusoidal nature of the wave-like pattern, that is of that respective orbifold eigenset -- that has here to have just had a Yukawa Coupling imparted upon it, -- to where the exhibition of its sinusoidal tendency of flow is here to have just become squared, -- will occur, in so as to then happen immediately, in this particular case, to behave in so as to bear a perturbative effect, from acting as an eigenfunction that was initially on the order of Appertaining To "i(sin((theta)(x,y)))", to then acting as an eigenfunction -- that is now to be on the order of Appertaining To "-(sin^2((theta)(z,y)))".  Since this particular perturbation of a wave-like pattern is both sudden and orthogonal, it will consequently tend to bear a spurious alteration in the perturbation of its energy-related path, -- since it will here be of a Hamitonian Operation, that will tend to cause a change in more derivatives than the number of spatial dimensions that the directly corresponding orbifold eigenset is here to be traveling through.  This will then tend to work to cause a set of Lagrangian-related Chern-Simons singularities to be formed.  Furthermore -- since this particular perturbation of a wave-like pattern, is to square in its sinusoidal oscillation-based tendency, -- it will tend to most certainly alter in its dimensional-related pulsation.  This will then tend to work to cause a set of metric-related Chern-Simons singularities to be formed.  To Be Continued!  Sincerely, Sam Roach.

Some Cool Stuff About Reverberation Invariants

Reverberation Invariants -- what are these?  Here is one unique general genus, as to what a person may sometimes mean -- when they are here to refer to the term "reverberation invariants," -- when this is here to be taken at the substringular level.  Let us look at a closed string, that is here to be of a symplectic geometry, to where such a said superstring is here to be altering in its motion -- when this is in terms of its relationship, relative to light -- over the course of one given arbitrary set of iterations of group-related instanton.  After a certain brief evenly-gauged Hamiltonian eigenmetric, -- those partitions, that are here to work to involve the condition of that homotopic residue -- that is here to be directly related to the Polyakov Action that is pertinent to the relative motion of the said respective superstring of discrete energy permittivity, are then to tend to alter in their relative delineation and scalar amplitude -- as is according to the re-adjustment of the motion of the said superstring, when in relationship to both the motion and the existence of electromagnetic energy.  In the process, the proximal local Fock Space, that is of the given arbitrary respective region, will then tend to metaphorically act like a "spring" of seemingly disoriented first-order point particles, that are here to act, in so as to work to transfer a reverberation effect, that may here be thought of as a tense of a rippling effect, -- along the topology of the said string.  Entropy tends to be caused by the scattering of electromagnetic energy.  The Gliosis-related impact that is here to be formed,when electromagnetic energy is to scatter upon phenomenology -- tends to form an eminent effect upon the directly corresponding externalized core-field-density of those light-cone-gauge eigenstates, that will have thence to have just been struck by photon-related energy.  Such a direct impact, will thence tend to work to effect those vibrations that are to be formed by the plucking of second-order light-cone-gauge eigenstates by their correlative gauge-bosons.  This just mentioned tendency, will then tend to work to perturbate the nature of those Schwinger-Indices -- that are thence to be formed by the earlier so-stated plucking effect of gauge-bosons upon the said second-order light-cone-gauge eigenstates.  The quantization of Schwinger-Indices, that are propagated in such a manner -- that is both transversal and perpendicular -- as well as being of such a nature, in so as to then to work to bear a wavelength that is anywhere from between 5*10^(-22) of a meter to 4*10^(-18) of a meter in scalar magnitude, are what may be thought of as being the phenomenology of gravitational waves.  The activity of the relatively consistently occurring mingling of such gravitational waves, when this is here to be fractaled down to a level that may be more directly Yukawa to a superstring of discrete energy permittivity -- that is here to interact upon the topology of discrete energy in a ripple-like manner, over time, is what I had meant by the phrase, "reverberation invariants."
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

More As To The Nature Of Light-Cone-Gauge Topology

Generally -- during any given arbitrary iteration of BRST -- when one is to have a discrete quantum of energy, that is to bear a Yang-Mills light-cone-gauge topology (non abelian) -- those second-order light-cone-gauge eigenstates, that are positioned at the immediately reverse-holomorphic side of the directly corresponding superstring of discrete energy permittivity, that is of such a respective case, -- when this is here to be taken at a level that is Poincare to the topology of the here mentioned individually taken second-order light-cone-gauge eigenstates, -- are here to tend to work to bear a relatively sinusoidal Laplacian-related delineation (like a relatively sinusoidal standing wave, that is being increased in its relative length -- by the activity of an increased scalar amplitude of mini-stringular segmentation -- that is being fed-into the relatively adjacent proximal locus), that are then to be plucked like a harp, at their correlative "troughs," by the directly corresponding gauge-bosons, -- in so as to work to produce those Schwinger-Indices, that operate via their propagated vibrations, in so as to help at working to do Their Part, at influencing the formation of the existence of the four general forces of nature.
Furthermore:  generally -- during any given arbitrary iteration of BRST -- when one is to have a discrete quantum of energy, that is to bear a Kaluza-Klein light-cone-gauge topology (abelian) -- those second-order light-cone-gauge eigenstates, that are positioned at the immediately reverse-holomorphic side of the directly corresponding superstring of discrete energy permittivity, that is of such a respective case, -- when this is here to be taken at a level that is Poincare to the topology of the here mentioned individually taken second-order light-cone-gauge eigenstates, -- are here to tend to work to bear a relatively supplemental Laplacian-related delineation (like a relatively supplemental standing wave, that is being increased in its relative length -- by the activity of an increased scalar amplitude of mini-stringular segmentation -- that is being fed-into the relatively adjacent proximal locus), that are then to be plucked like a harp, at the correlative alterations that are of a proximal local change in the first-derivative (where there is ulterior mini-stringular segmentation touching it), of such a so-eluded-to wave, by the directly corresponding gauge-bosons, -- in so as to work to produce those Schwinger-Indices, that operate via their propagated vibrations, in so as to help at working to do Their Part, at influencing the formation of the existence of the four general forces of nature.  To Be Continued!  To Be Continued!  Sincerely, Samuel David Roach.

My Current Understanding As To How Gravity-Based Cohomology Is Transferred

The cohomology that is thus formed, by those particles that I had mentioned in my last post, -- as being either "gravitons" (transversal-based) or "gravitinos" (radial-based) -- is to here be indirectly translated to the corresponding cite of the gauge-bosons, in such a manner, to where, as the said gauge-bosons act in so as to pluck the directly corresponding second-order light-cone-gauge eigenstates like a harp, there is then to exist, the general tendency, to where such a so-eluded-to tense of a set of translated cohomological eigenindices -- are to then to be transferred to the thence formed Schwinger-Indices, in so as to help at working to form those integrative set of Schwinger-Indices, that are to move in such a manner, that is simultaneously transversal and perpendicular, to where the wavelength of such a so-eluded-to wave, is to have a wavelength that is to be anywhere from and including (5*10^(-22) of a meter To 4*10^(-18) of a meter) in overall length, -- in such a manner, -- to where there is here to tend to be the transference of a translation of the cohomology of what I earlier named of as being "gravitons" and "gravitinos," to where such a so-eluded-to tense of a gravitational wave, is here to work to each bear only a wave-based knotting equation, without it working to bear a particle-based knotting equation.  The holonomic substrate of the transversal motion of a gravitational wave, works to help at describing the knotting equation -- that is related to the cohomology of a "graviton," whereas -- the holonomic substrate of the perpendicular motion of a gravitational wave, works to help at describing the knotting equation -- that is related to the cohomology of a "gravitino."
One may metaphorically think of the genetic translation of traits in biology.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Schwinger-Indices -- A Little As To Grand Unified Field Theory

That same general genus of phenomenology, that works to coalesce into waves that are to range from being between 5*10^(-22) meters in length up to 4*10^(-18) meters in length -- of which are that general form of Schwinger-Indices, that are formed by the plucking of second-order light-cone-gauge eigenstates by their respective gauge-bosons, in so as to work to form gravitational waves -- happens to be that same general genus of phenomenology, that is to interact with the many various Ward-Cauchy-related entities that exist in the substringular -- when this is here to be taken along the multiplicit array of the Rarita Structure, -- in so as to work to form the many faceted exhibitions of the four general genre of the physical forces of nature, -- these being: 1) The Strong Force, 2)  The Electrostatic Force,
3)  The Gravitational Force, &, 4)  The Weak Force.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.
                                                                                                     

A Little Bit About Flux Density

Let us here consider the multiplicit array of magnetic flux density eigenstates -- when this is taken in terms of the substringular.  An entity of a magnetic flux density, consists of multiple -- when globally distinguishabley speaking -- adjacent magnetic waves, that, through vibration, may extend the reach of their electromagnetic influence, over the span of some respective covariant bearing of time.  Yet, their correlative composite magnetic waves, that may here be adjacent to our extrapolation-related observance -- may actually be more separated than we would like to initially perceive these as being, if one were to consider the overall delineation of some of such waves, -- when all of the directly corresponding Lorentz-Four-Contractions are to be theoretically counted out of the scenario for a "time being."  Furthermore -- in a closest to an absolute tense, the Ward-Cauchy-related conditions, that are here to work to determine the boundary conditions at a microscopic set of considerations,  are here to be of the hierarchy -- as to how things are to actually behave in the realm of the substringular.  So, in a more real sense than the globally distinguishable, individual waves that are propagated from the source of a magnetic flux density -- may be separated over the course of taking the considerations of a Laplacian set of extrapolation-related conditions, even though all of the correlative waves that are to extend from a phenomenology that may here be considered to be of a magnetic flux density, are to be of one Gaussian-based eigenmatrix.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part One Of Session 13 Of Course 20

Electromagnetic energy, including all light, tends to scatter at least to some extent -- if that electromagnetic energy is not propagated in a perfectly orthogonal nature upon any given surface of any phenomenon that the given electromagnetic energy is interfacing upon.  Whenever any electromagnetic energy is orthogonal in both its transference and in its propagation through and/or upon a surface or region, the given electromagnetic energy is then here to be polarized, through and/or upon the given surface or region.  When electromagnetic energy -- in the form of quantized beams or waves -- is to be made orthogonal as a field, to any plain kinetic energy that is here to exist as a field, then, the said electromagnetic energy will tend to be absorbed, -- as opposed to instead being scattered.  If the given electromagnetic energy is not completely polarized, and is thus scattered, then, the electromagnetic energy that is here to be striking a tense of plain kinetic energy, must switch in its genus of light-cone-gauge topology -- right after the so-eluded-to light acts in so as to strike the surface of the given plain energy of such a given arbitrary case.  That would then mean, that the said electromagnetic energy that is scattered here, is then here to change temporarily from initially working to bear a Yang-Mills topology, into then working to bear a Kaluza-Klein topology.  This here would then mean, that the Clifford algebra here would convert from working to primarily bear both a euclidean and a hermitian geometry, into then working to involve primarily a euler and a Dirac geometry -- for the time being.  Once the given electromagnetic energy is scattered, the Gaussian of the stringular part of the light, will then switch in light-cone-gauge orientation by 90i degrees.  The torque given in the Gaussian, causes a spring-like torsioning, that is here to automate a reversal in the changed Gaussian.  As the Gaussian is switched by the said light-cone-gauge torsioning, the scattered electromagnetic energy is then to work to pull in upon itself -- to act in so as to work to cause the scattered light to requantize with the proximal local Yang-Mills topology -- that is in the here so-eluded-to substringular region.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.