Priming To Help Facilitate The Formation Of Energy/Force

 Just as electromagnetic energy works to help prime the Rarita Structure, in so as to assist in facilitating the formation of the reductional energies of physical nature; Neutrinos work to help prime the Rarita Structure, in so as to assist at facilitating the formation of the reductional forces of physical nature. SAMUEL DAVID ROACH. 

A propagated, cohomology-based topological manifold, that works to exhibit, a succinctly recursive, diffeomorphic pattern, of projected trajectory, may often tend to be formed, by a Kahler Hamiltonian Operator, that generates as much cohomology as it de-generates, as taken, time wise, in a very piecewise continuous manner. 

The non perturbative oscillation-based eigenstates, of the Lagrangian-Based motion, of a spinning Mass-bearing Kahler Hamiltonian Operator, of which is here to be recursively re-calibrating, in its net Chern-Simons Invariant relationship, may often tend to be eminently associated, with facilitating, a viable delineated tense, of physically generated charge. Whereas; The perturbative oscillation-based eigenstates, of the Lagrangian-Based motion, of a spinning Mass-bearing Kahler Hamiltonian Operator, of which is here to be recursively re-calibrating, in its net Chern-Simons Invariant relationship, may often tend to be eminently associated, with facilitating, a viable delineated tense, of physically generated entropy.  

Again; Chern-Simons Invariants are only actually invariant, when both the speed And the direction, of an eminently associated Kahler Hamiltonian Operator is to stay the same. So, if a Kahler Hamiltonian Operator, is to be constantly spinning, its eminently associated Chern Simons Invariants, will consequently be constantly re-calibrated.  

A kinematically delineated, gauge-invariant Kahler Hamiltonian Operator, may often tend to express a steadier pulse, than an otherwise analogous Kahler Hamiltonian Operator, that instead, is not gauge-invariant.

A gauge-invariant Kahler Hamiltonian Operator, generally tends to have a greater probability, of working to bear an isotropically stable nature, than an otherwise analogous Kaher Hamiltonian Operator, that instead, is not gauge-invariant.   

The transversal propagation, of a given arbitrary, kinetically transferred, mass-bearing, Kahler Hamiltonian Operator, tends to eminently work to involve, the Euclidean-Based Expansion, of its net Lagrangian-Based motion. Whereas; The radial propagation, of a given arbitrary, kinetically transferred, mass-bearing, Kahler Hamiltonian Operator, tends to eminently work to involve, the Clifford-Based Expansion, of its net Lagrangian-Based motion. When the Lagrangian-Based Expansion, of a kinematically propagated, Kahler Hamiltonian Operator, is heuristically augmented, this may often tend, to be eminently associated, with the covariant proximal local presence, of a Slater-Based Incursion, when Gliosis to the externalized field-density, of its respective motion. Whereas; When the Lagrangian-Based Expansion, of a kinematically propagated, Kahler Hamiltonian Operator, is heuristically diminished, this may often tend, to be eminently associated, with the covariant proximal local presence, of a Poincaré-Based Incursion, when Gliosis to the externalized field-density, of its respective motion. 

The metric component, that is inextricably in association, with the multiplicity of pulsation, that may be perceived of here, to be in lieu, of the kinetic transference, of a cohesive set, of discrete mass-bearing eigenstates, may often tend to fundamentally emanate, the physically demonstrative, kinematic attribute, of the resolution, of the  implicit, eminently associated, Kahler Hamiltonian Operator, that is here to be taken into consideration. Moreover; The heuristic component, that is inextricably in association, with the multiplicity of pulsation, that may be perceived of here, to be in lieu, of the kinetic transference, of a cohesive set, of discrete mass-bearing eigenstates, may often tend to fundamentally emanate, the physically demonstrative, kinematic attribute, of the succinctness, of the implicit, eminently associated, Kahler Hamiltonian Operator, that is here to be taken into consideration.  

The pulse of physical imagination eigenstates, when this is taken into perspective, in lieu of the eminently associated kinetic energy that is tugging it in a relatively holomorphic manner, when taken through its directly associated Lagrangian, may often tend to work to facilitate, the homotopic transfer, of the implicit tense of autonomy-related eigenstates, that are here to be in the general process, of being kinematically propagated over time.  

A (smooth) Real Riemann-Based cohomology-related flow, of Lagrangian-Based motion, will tend to be hermitian, to where it will often tend to work to bear no Chern-Simons-Related cohomology-based spurs, over the covariant kinematic course, of its mappable-tracing.  

The hermitian pulsation, of a hermitian compact topological manifold of quantum energy, may often tend to work to form, a hermitian Fourier-Related-Progression. 

 The more strongly gauged that the thought energy is to be, that is here to be spontaneously interacting with a topological manifold of inertial-related pulsation, the more spontaneously resolute that the resulting time will be, of which is here to be consequently generated, by the implicit  kinematically propagated interaction, that is thence to spontaneously tend to ensue in its occurrence, subsequent to the implied interface that is to be incurred, between the stated tense of thought energy, when in corroboration with the stated tense of inertial-related pulsation, over time.  

A Kahler Hamiltonian (Operator), that works to bear a relatively strong resolute Fourier-Related-Progression, may often tend to impart, a spontaneously significant “push” through space. Whereas; A Kahler Hamiltonian (Operator), that works to bear a relatively strong succinct Fourier-Related-Progression, may often tend to impart, a spontaneously significant “glide” through space.  

A Yang-Mills-Related Topological Manifold, tends to be kinematically propagated, from a relatively internal reference-frame. Whereas; A Kaluza-Klein-Related Topological Manifold, tends to be kinematically propagated, from a relatively external reference-frame.  

Anti gravity, may often tend to reverse the holomorphic flow, of a covariant tense, of an eminently associated cohesive set, of corroborative yin(g)/yang eigenstates.

The Drive of the covariant, kinematically propagated, physically projected delineation, of the Fourier-Related-Progression, of a kinetically transferred, Kahler Hamiltonian Topological Manifold, may often tend to be described of, as the gauged assertion, of the commutative extension, of a set of one or more interactive cohesive wave-fronts, as spontaneously conjecturable in the Ward-Cauchy-Related Realm. Such a drive, may often tend to be communicated of, as being analogous, simply, to the pulsation of the implicit team of eigenstates, per its energy. 

Diminishing Propagated Beam Of Light -- Clifford-Related Torsion -- Slater-Related Recursion

 A propagated beam of light, of which is here to be steadily diminishing in its field intensity, may said to respectively tend to be spontaneously enacted upon, by a Clifford-Related torsion. The recursively considered torsion, that is here to be heuristically enacted, upon such a beam of electromagnetic energy, in so as to work to facilitate such a steadily diminished hereupon inferred electromagnetic field intensity, may be said to often tend to work to be inherently related, to a directly associated Slater-Related recursive field operation, as taken over a directly corresponding respectively potential proscribed duration of time. SINCERELY, SAMUEL ROACH.

Part One Of Gravitational Topological-Variance

 When an electron is struck by a beam of electromagnetic energy, it (the electron), will tend to fall back-and-forth an energy level -- to where the resultant residual spare energy, that is here to be respectively incurred upon the covariant Ward-Cauchy-Related bounds of such a stated electron, is to consequently be released, as a tangentially propagated discrete quantum of electromagnetic radiation. Right around the moment, during which a beam of electrodynamic radiation, is initially to come into a direct contact, with the holonomic stratum of the core-field-density of an electron, (of which is to be about 7*10^(-17) of one second after the immediate Gliosis-Based contact), the interaction between the inferred beam of photons with the topological stratum, that is here to be of the core-field-density of the electron, to where the shape of the topological contour, of that gravitational field, of which is here to work to bear an eminently associated covariant immediately externalized relationship, with the topological field that is proximal local to the core-field-density of the herein stated electron, is to alter in its directly associated topological morphology, to where such an inferred gravitational field, that is here to be directly corresponding to the said electron that I have eluded to here, while in mentioning such a respective given arbitrary type of a case scenario, is thereby to consequentially vary in the delineation-related distribution of its directorial-related construction, to where such a general genus, of the correlative alteration in the directorial-related contour of such an inferred topological gravitational field, may consequently be said, to be undergoing the general process, of what I call, the reductional operational-related Ward-Cauchy-Related physical condition, of what may consequently be called, the Gravitational Topological-Variance. (GT).

Let us next say, that the electron-related co-tangential bundle that is being approached, by the earlier eluded-to beam of electrodynamic radiation, is here to be of an arbitrary spatial dimensionality, of N dimensions. (It may be anywhere from co-tangential bundle R3, to co-tangential bundle R6). The equation that I have recently come-up with, for working to help determine what the Gravitational Topological-Variance, is, for the case of an initially scattered electron, of which is here to be proximal local in its eminent presence, after about 7*10^(-17) of one second upon the initial immediate contact of the inferred electromagnetic energy with the eluded-to respective given arbitrary electron that is here to be beginning to be scattered, as taken at the Poincare level to the immediate region of direct interaction, is:

GT(v) = ~ {[[The Ricci Flow]*[((N-1)*e^((2*(1-N)) - 1]*[((N-1)*e^((2*(1-N)) +1]]

*(((N^.5)/N)*((e^(The Ricci Flow))^6) {+ - (I hat), + - (j hat), + - (k hat), ... + - ( q(n) hat)}.

To where, the "hat" term, is here to elude to a reference, to the reductional shape-based delineation-related distribution, that is here to be constructed, via an understanding of the Laplacian-Based direction(s), of which are here to be directly related to the mappable contour of the shape of the directly correlative gravitational field, that is here to be expressed, at the eminent proximal local region, that is immediately externalized to the core-field-density, that is here to be directly associated with the eminently correlative electron, that is here to be of such a respectively given arbitrary type of a case scenario. SAMUEL. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! 

The Fourier-Related-Progression Of The Homotopic Translation Of Component Light-Cone-Gauge Eigenstates

 When electromagnetic energy scatters, the Fourier-Related-Progression, of the homotopic translation, of the associated proximal local respective component light-cone-gauge eigenstates, is to tend to work to bear, an anharmonic perturbation. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH.

Electromagnetic Energy Interacting With Mass-Bearing Light-Cone-Gauge Eigenstates

 When electromagnetic energy is to interact with a Noether-Based mass-bearing light-cone-gauge eigenstate, in a Glosses-Related manner, this will often tend to work to form a perturbation, in the distributional delineation, of the said light-cone-gauge eigenstate. SAMUEL DAVID ROACH.

Inversion Of The Fujikawa Coupling Via The Green Function

 As to what may here be theoretically logically deduced; When the Inversion of the general operational processes, that are here to be directly appertaining to the general kinematic flow, of the Fujikawa Coupling via the Green Function, is to occur in such a manner, to where it is here to be incurred, upon the topological manifold of the Ward-Cauchy-Related field density, of a superstring of discrete electromagnetic energy permittivity, it is consequently to follow, that such a general genus of a Ward-Cauchy-Related kinematic operation, may be perceived of, as working to bear the general tendency, of often bearing a high probability, of consequently directly altering the metric-based structure, as well as less directly working to alter the directly associated operation, of such an inferred photon, in such a manner, to where such an inferred perturbation in both the structure and operation, of what was here to initially have been a superstring of discrete electromagnetic energy, to now, in such a given arbitrary case, to become a respective consequentially resultant superstring of discrete kinetic energy permittivity. SINCERELY, SAMUEL (1989).

As To The Cyclical Metric Flow Of Anti-Gravity

 The cyclical metric flow of anti-gravity —  may often be able to alter the dimensional-related pulsation, of a directly contingent set of discrete electromagnetic energy quanta. To Be Continued!!!  Samuel Roach.

Cool Stuff As To The i*PI(del) Action

 The i*PI(del) Action, is the action of a change, in either the number and/or in the delineation, of those partition-based discrepancies, — that are here to be directly associated, with the physical condition, in which a super string of discrete energy permittivity, is to alter in its motion (when in terms of either its speed and/or in its direction), in its relationship to the motion of electromagnetic energy. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (PHS 1989).

More As To The Perturbation Of Chern-Simons Invariants

Whenever any given arbitrary mass-bearing orbifold eigenset is to not be changing in its relative motion, when this is here to be taken in its relationship to both the motion and the presence of electromagnetic energy --  its Chern-Simons Invariants will then consequently tend to not alter (perturbate), or, in other words, these particular Chern-Simons Invariants will then consequently tend to remain "invariant." Sincerely, Samuel David Roach.

The i*PI(del) Action Not Eminent, And Even Velocity

Whenever any one given arbitrary mass-bearing orbifold eigenset, is to work to maintain the same rate of motion as taken in a constant direction -- when this is here to be taken in its relationship to both the motion and the existence of electromagnetic energy, -- then, the directly corresponding i*PI(del) Action, that is here to be correlative to the relativity of the said respective given arbitrary orbifold eigenset of such a case scenario, will tend to not be eminent in its general tense of activity. I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

A Brief Editorial About Light Speed

As an initial ansantz, light is the prime example that one is to generally think of -- when one is here to be talking about electromagnetic energy.  Light in a vacuum on earth -- when this is here to be taken into consideration of, by both the motion and the gravitational influences of our said earth, to where such inferred influences are here to work to effect the relative rate of such light -- works to help such said light, to travel at a velocity of 2.99792458*10^8 meters per second, under the just implied Cauchy-related conditions.  The fastest speed that electromagnetic energy (when not including Kirchoff Radiation), is capable of traveling at in a vacuum, is at a rate of 3*10^8 meters per second.  Furthermore -- the overall average rate in which light may be propagated at through a vacuum, -- is at a rate of 2.999999985*10^8 meters per second.  To Be Continued!  Sincerely, Samuel David Roach.

Mass-Bearing Nodes

When any one given arbitrary Noether-based orbifold eigenset is to increase in its velocity in relation to electromagnetic energy, those individually taken superstrings of discrete energy permittivity that work to comprise such a said eigenset, are consequently to tend to increase in their attribution, as a set of mass-bearing nodes in time and space.  As a Noether-based superstring of discrete energy permittivity is to increase in its attribution as a mass-bearing node, it will consequently tend to work to bear less, of what I term of as being "partition-based discrepancies."  As such a Noether-based superstring of discrete energy permittivity is to increase in its velocity, in relation to electromagnetic energy, it will increase in its Lorentz-Four-Contraction -- and thereby decrease in its directly corresponding Polyakov Action.  This is part of the reason as to why a Noether-based superstring with a relatively lowered Polyakov Action, will tend to bear less partition-based discrepancies.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Altering Rate Of i*PI(del) Action

When a given arbitrary mass-bearing orbifold eigenset is to be altering in its acceleration, when this is here to be taken in its relationship to the velocity of electromagnetic energy -- then, the correlative i*PI(del) action that is here to be directly corresponding to the said respective given arbitrary mass-bearing orbifold eigenset, will consequently tend to be altering in its rate.  Sincerely, Sam Roach.

Some Stuff As To The Speed Of Light

You know how electromagnetic energy (light) in a vacuum -- from within the realm of our planet -- travels at a velocity of 2.99792458*10^8 meters per second?  Our planet spins on its axis, and also orbits around our sun in an elliptical manner.  Both our solar system as well as our galaxy, is moving as a unit, -- through the fabric of space and time.  Did it consequently ever occur to people that fundamental electromagnetic energy, in the realm of any given vacuum to be considered here to exist in deep outer space -- may then often actually travel at exactly 3*10^8 meters per second?
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Release Of Relative Yukawa Bearing

When the general Ward-Cauchy-related process is here to be going on, during which the residual kinetic energy of an electron is to be released in the form of a photon -- there is here to be one directly corresponding open-looped superstring of discrete energy permittivity, that is then to release the immediately prior state that it had had, when in terms of its relative Yukawa bearing upon the correlative respective electron, to where right after such a said general process is to occur -- the here just released correlative discrete quantum of a Legendre homology, is then to undergo the general process,  that is here to be directly involved with the activity of the Fujikawa Coupling,  which is here to happen via the manner of activity that is known of as being of the Green Function, -- in so as to ensue as to work to form one given arbitrary respective discrete quantum of electromagnetic energy.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Direction Of The General Forces Of Nature

Whenever electromagnetic energy is to scatter upon another phenomenology,  one or more discrete quanta of electromagnetic energy are here to be striking the externalized core-field-density of the respective coresponding light-cone-gauge eigenstates in a Gliosis-based manner, -- in so as to work to influence the general flow of the directly corresponding proximal local Schwinger-Indices.  Consequently, this general genus of an interaction that is here to be happening between discrete quanta of electromagnetic energy and the light-cone-gauge is to then to be able to work to influence the general direction in which the forces of nature are to be applied.
Samuel David Roach.

Fluctuation In Electric Field

The wavelength of a beam of any given arbitrary tense of electromagnetic energy, is equal to one complete oscillation of the fluctuation of the directly corresponding respective electric field.
Here's one way of looking at what is here to be meant by "the fluctuation of the directly corresponding electric field."
Let us consider a metaphorical "shaft of brightness," that is here to be at one given arbitrary maximum cross-sectional measure of thickness, for such a so-eluded-to beam.  Let us now say that this said respective shaft, is here to be traveling in a vacuum -- to where it will be propagated, in so as to be traveling as straight as the general innate bending of space and time is to be designated-- along the general course of space and time.  As this said "shaft of brightness" is to be propagated along the general course of space and time -- the so-eluded-to projected beam of brightness, that is here to be linearly delineated, will then tend to go from smoothly decreasing in its cross-sectional thickness, to then going into smoothly re-gaining its initial so-eluded-to cross-sectional thickness, and back again.  In the meanwhile, the center of such a harmonic tense of a fluctuation is to be going as perfectly straight -- as the natural bending of space and time will tend to allow. The scalar distance that is to be considered here, as being taken along the vantage-point, of an extrapolation that is here to be Poincare to the topology-related center of such a so-named shaft of brightness, in which there is here to be the completion of one whole individually taken tense, of the earlier mentioned harmonic perturbation in the cross-sectional thickness of the so-eluded-to beam -- may be here to be analogous to what is meant -- as to what is here to be happening to a beam of electromagnetic energy, as it is here to be harmonically fluctuating in its electric field over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Electricity And Partition-Based Discrepancies

With electricity, there is energy per charge before there is charge per time.  Voltage happens before there is amperage.  Voltage is more in reference to the magnetic field, while amperage is more in reference to the electric field.  Per instanton, the just mentioned tendency fractals down to the condition, that an orbifold eigenset of electromagnetic energy is to gain partition-based discrepancies before it is to lose the exact same number of such said partition-based discrepancies.  The magnetic field is thus indicative of that fluctuation in electromagnetic energy, that is due to an increase in the Hodge-Index of the holonomic substrate of discrete homotopic residue, in the form of a transient gain of partition-related discrepancies, -- while the electric field is indicative of that fluctuation in electromagnetic energy, that is due to a decrease in the Hodge-Index of the holonomic substrate of homotopic residue, in the form of a transient loss of partition-related discrepancies.  The Fourier-related integration of such a generation/degeneration of partition-related discrepancies, is what is here to work to form what here may be thought of as the correlative respective magnetic field eigenstates & the correlative respective electric field eigenstates.  Just as the condition that electromagnetic energy is reverse-fractaled as electromagnetic wavelengths, both magnetic and electric field eigenstates are, in a way, a reverse-fractal of the flow of the exchange of partition-based discrepancies.  The manner by which magnetic field eigenstates are not overcome by electric field eigenstates, -- is that the magnetic field works to curl around the electric field, as is in accordance with the right-hand-rule, in a manner that is not only both covariant, codeterminable, and codifferentiable, yet, such a Yukawa-related curling of electromagnetic eigenstates upon one another, is to happen here in an accordance with the drive of that angular momentum -- that is here to tend to be in the general direction of the relative forward-holomorphic topological wave-tug of any given arbitrary respective case in point.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two Of Session 13 Of Course 20

By the way, -- the general condition of the torsion that alters the order of any one said light-cone-gauge eigenstate by 90i degrees, works to cause the correlative composite second-order light-cone-gauge eigenstates to either go from working to bear a sinusoidal delineation -- to working to bear a relatively supplemental delineation, when there is a light-cone-gauge perturbation that is to go from working to exhibit a Yang-Mills or non abelian light-cone-gauge topology, to working to exhibit a Kaluza-Klein or abelian light-cone-gauge topology, or, in the ulterior case, to cause the composite second-order light-cone-gauge eigenstates to go from working to bear a relatively supplemental delineation, to working to bear a sinusoidal delineation, when there is a light-cone-gauge perturbation that is to go from working to exhibit a Kaluza-Klein or abelian light-cone-gauge topology to a Yang-Mills or non abelian light-cone-gauge topology.  Such a said torsioning is necessary, in order to work to allow for electromagnetic energy to initially to be able to re-arrange as entropic photons, when it is first disorganized by a correlative scattering -- while to then to be able to re-group and re-quantize as non entropic photons, once such electromagnetic energy has torsioned back into the general genus of the proximal local electromagnetic radiation.  Once the multiplicit photonic energy is to be re-quantized back into the general proximal local electromagnetic radiation, in so as to here to be having a Yang-Mills light-cone-gauge topology -- its Clifford algebra will then have more of a tendency of going from working to bear a primarily euler and a Dirac geometry, into working, instead, to bear a primarily euclidean and a hermitian geometry, over time.
 I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Homotopic Residue And Light

The delineation of all homotopic residue that is of mass-bearing superstrings, is relative to both the motion and the existence of electromagnetic energy -- or, to paraphrase this -- the delineation of all homotopic residue, is relative to both the motion and the existence of light.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.