Interaction Of Higgs Action With Anti-Holomorphic Energy Quanta

 The general interaction of the gauging of the Higgs Action, With the general topological sway of a given arbitrary respective cohesive set of discrete energy quanta, that has just started to initiate into a tense of working to display a set of anti-holomorphic Kahler conditions, tends to work to form the genus of a type of a gauged-action, that may here be described of, as being the Wick Action. SAMUEL ROACH. (1989).

Higgs Boson Eigenstate — Anti-Holomorphic Kahler Conditions

 The general effect of the multiplicity of the Higgs Boson eigenstate, tends to be delineated to those given arbitrary regions, all over space-time-fabric, — at which anti-holomorphic Kahler conditions are to be initiated. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

A Cool Editorial — As To The “Driving-Force” Of Space-Time-Fabric

 I surmise, that the general net “pulse” of the Multiverse, — may be thought of, as being of the following manner of nature:

The multiplicity of pulsation in the Multiverse, is the “driving-force” of space-time-fabric, per permutative cohomology-related generation. 

I will continue with the suspense later! To Be Continued!  Sincerely, SAMUEL DAVID ROACH. (1989).

“Ablated” Homotopic Residue — My Perception

 If one were to take the inversion of the process, of the general gauged-action, of a Noether-based unitary homeomorphic escalating Lagrangian of a Euclidean expansion, one would then tend to have, instead, the process, of the general gauged-action, of a Noether-based unitary homeomorphic attritional Lagrangian, that is of a Euclidean contraction, to where, instead of such a said Lagrangian working to bear a compounded tense of homotopic residue, such an attritional Lagrangian, would consequently tend to work to bear an “ablated” tense of homotopic residue. I will continue with the suspense later! Sincerely, SAMUEL DAVID ROACH. 

I*PI(del) Action Eminence — Relative Motion

 Whenever a cohesive set of discrete energy quanta, is to alter at all in its relative motion, when this is here to be taken, in its relationship to electromagnetic energy, — four different things will consequently always tend to be happening: 1) It will tend to work to bear the tense of some sort of a Lorentz-Four-Contraction.

                            2) It will tend to perturbate in a set of one or more Chern-Simons Invariants.

                            3) It will tend to work to bear an eminent i*PI(del) Action. 

                       &, 4) It will tend to Lack gauge-invarince.

‘Till next time! To Be Continued! Sincerely, SAMUEL DAVD ROACH!

The i*PI(del) Action — Gauge-Invariance

 When the i*PI(del) Action is not to be physically eminent, for the workings of a given arbitrary mass-bearing cohesive set of discrete energy quanta, — then, one may tend to say, that such a said respective mass-bearing cohesive set of discrete energy quanta, is then to work to bear the condition of being “gauge-invariant.” I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL ROACH. (1989).

Escalating Lagrangian — Chern-Simons Singularities, — My View

 Those Lagrangian-based Chern-Simons singularities, that are thence to tend to be formed, by the gauged-action of the heteromorphic escalation of a correlative Lagrangian, that is here to be of a Clifford Expansion, tend to bear an anharmonically permutative tree-based nature; whereas, — those Lagrangian-based Chern-Simons singularities, that are thence to tend to be formed, by the gauged-action of the heteromorphic escalation of a correlative Lagrangian, that is here to be of a Euclidean Expansion, tend to bear an anharmonically permutative commutative-trace-based nature. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

Inverted Compounded Homotopic Residue

 If one were to take the anti-derivative of the unitary homeomorphic escalating Noether-based Lagrangian, that is here to be of a Euclidean Expansion, one would then tend to work to be mathematically depicting a situation, to where one is then to be considering, instead, the steady-state gauged-action of the Fourier-Transform, of the correlative inferred Lagrangian-based eigenstate, that is thence to be homotopically comprised of, by the holonomy of the inferred kinetically driven cohesive set of mass-bearing discrete energy quanta, of such a respective given arbitrary case. This would also work to depict, a consequentially resultant inversion, to the prior inferred proximal local presence, of the correlative compounded homotopic residue. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Compounded Homotopic Residue — Asymptotic Divergence

 The more that the homotopic residue of an escalating Lagrangian, that is here to be of a Euclidean expansion, is to be compounded, over a given arbitrary proscribed duration, that is here to be of a sequential series of group-related instantons, the more that the corresponding pertinent Euclidean tangential bundle(s) directly involved, will consequently result, in tending to diverge in more of an asymptotic manner. The more that the homotopic residue of an escalating Lagrangian, that is here to be of a Clifford expansion, is to be compounded, over a given arbitrary proscribed duration, that is of a sequential series of group-related instantons, the more that the corresponding pertinent hyperbolic tangential bundle(s) directly involved, will consequently result, in tending to diverge in more of an asymptotic manner. I will continue with the suspense later! Sincerely, SAM ROACH. (1989).

Escalating Lagrangian Of Euclidean/Clifford Expansion, Doesn’t Tend To Exhibit A Flat Ricci Curvature

 Any Noether-based mass-bearing cohesive set of discrete energy quanta, that is here to work to be displaying an escalating Lagrangian of a Euclidean/Clifford Expansion, during this process of such an inferred tense of an escalation,  will tend to not be capable of  working to exhibit the general physical condition, of bearing a flat Ricci Curvature. Sincerely, SAMUEL ROACH. (1989).

Compounded Homotopic Residue

 In general — a binary homeomorphic escalating Lagrangian, that is here to be undergoing a Euclidean/Clifford Expansion, tends to work to exhibit a greater scalar attribute, of a proximal local tense of compounded homotopic residue, than a unitary homeomorphic escalating respective Lagrangian, that is here to be undergoing a respective Euclidean/Clifford Lagrangian does; a tertiary homeomorphic escalating Lagrangian, that is here to be undergoing a Euclidean/Clifford Expansion, tends to work to exhibit a greater scalar attribute, of a proximal local tense of compounded homotopic residue, than a binary homeomorpjhic escalating respective Lagrangian, that is here to be exhibiting a Euclidean/Clifford Expansion does; etc... . I will continue with the suspense later! Sincerely, SAMUEL DAVID ROACH.

Photons And The Kahler-Metric

 Whenever a Noether-based photon is to scatter upon a phenomenon, it is thereupon consequentially to tend to immediately become Gliosis to the Kahler-Metric. Sincerely, SAMUEL DAVID ROACH. (1989).

Tree-Based Directorals Versus Commutative-Trace-Based Directorals

 The mathematical description of a given arbitrary escalating Lagrangian, that is here to be of a Clifford Expansion — tends to work to bear a set of tree-based Directorals; whereas, the mathematical description of a given arbitrary escalating Lagrangian, that is here to be of a Euclidean Expansion — tends to work to bear a set of commutative-trace-based directorals, — in the process of working to describe the flow of the cohomology, that is here to be of the correlative cohesive set of discrete energy quanta, that is here to be exhibiting the said Lagrangian, that is thence to be escalating in its general scalar attribute. SAM ROACH.

“Wear-And-Tear” Upon A Worm-Hole

 The multiplicity of the general interaction, of entropic tachyon-related photons (which tend to bear the combination, of having both a Khovanov geometry, along with a  Kaluza-Klein light-cone-gauge topology), with discrete energy quanta, that are here of the nature of working to bear a tachyon-related tense of kinetic energy (which tend to bear the combination, of having both a Khovanov geometry, along with a Yang-Mills light-cone-gauge topology), — works to facilitate the general processes, by which the “wear-and-tear,” that is here to be attributable, to what may often tend to happen to a worm-hole, when it has been utilized enough times, is often thereby to be able to happen to such a space-time-related “shortcut,” if it has been exacerbated, over the potential combination of both a lot of usage, along With a long duration that it may have been present, at some given arbitrary covariant region of space. Sincerely, SAMUEL DAVID ROACH.

Inextricable Inter-Relationship, Between General Tenses Of Symplectic Topological Manifolds

 The inextricable exhibition, of the multiplicity of that general kinematic interplay, which is of those Ward-Cauchy-related phenomenology, that are here to display the general physical conditions of Noether Flow —  to where such an exhibition is thence to exist, between/amongst the Fourier-related translational differentiation, that is here to be of the general tense of superstring-related symplectic topological manifolds, that are here to work to bear a Kaluza-Klein light-cone-gauge topology, With, the Fourier-related translational differentiation, that is here to be of that general tense of superstring-related symplectic topological manifolds, that are here to work to bear a Yang-Mills light-cone-gauge topology,— tends to work to facilitate the general panoply of the multiplicity of interaction, by which the physical conditions of space-time Relativity, are consequently to result in taking hold, upon the inextricable relationship that is here to exist — amongst the attributable alterations, that are of the relevant characteristics of mass-based phenomenology, as the motion of mass is to bear any sort of variance, when this is here to be taken, in its relationship to the pertinent motion of electromagnetic energy. To Be Continued! Sincerely, SAM.

Harmonics Of Pressurized Vacuum Perturbation

 The general harmonic perturbation, of a given arbitrary tense of a Ward-Cauchy-related pressurized vacuum, tends to “move” in the “direction,”of inclining those effected discrete quanta of energy, that are thence to be directly influenced, by such a general genus of a given arbitrary tense of a harmonic perturbation, — to have an increased probability of tending to work to form the physical conditions, of working to bear a Riemann Scattering; Whereas — the general anharmonic perturbation, of a given arbitrary tense of a Ward-Cauchy-related pressurized vacuum, tends to “move” in the “direction,” of inclining those effected discrete quanta of energy, that are thence to be directly influenced, by such a general genus of a given arbitrary tense of an anharmonic perturbation, — to have an increased probability of tending to work to form the physical conditions, of working to bear a Rayleigh Scattering. SAMUEL.

Perturbative Pressurized Vacuum — Topological Sway

 Let us initially consider two different and distinct superstrings of discrete energy permittivity, that are here to be basically of the same nature, — except, that one of such individually taken superstrings, is to exist in an environment, that is here to work to bear a greater scalar amplitude of a tense of a perturbative pressurized vacuum enacted upon its topological stratum,  than the other inferred superstring of discrete energy permittivity is thence to be existent in, ( to where the second inferred superstring of discrete energy permittivity, is here to work to bear a lower scalar amplitude, of a tense of a perturbative pressurized vacuum that is here to be enacted upon it), — as this is here to be taken, over a simultaneous durational course (via the vantage-point of a central locus), that is of a common proscribed given arbitrary tense, of the workings of a directly corresponding Fourier-related Transformation (as this is here to be taken, over a common relativistic and respective covariant duration of time). That superstring of discrete energy permittivity, that is to be existent in an environment, that is here to be exhibiting a greater scalar amplitude of a tense of a perturbative pressurized vacuum enacted upon it, will consequently tend to bear a greater scalar amplitude of topological sway (as in terms of the oscillation-related flow of its “regional-swipe-inhabitation”), than the other of the two individually taken superstrings of discrete energy permittivity will tend to be exhibiting — as this is here to be taken, over an evenly-gauged Hamiltonian eigen-metric. SAM. 

Escalating Lagrangian — Isotropic Spur

 When one is to have a given arbitrary escalating Lagrangian of Euclidean/Clifford Expansion, that is here to work to bear a mappable isotropic “spur,” at a semi-set locus that is Virtually of a pure Laplacian-related nature, as this is here to be mapped-out, along the path of the inferred determinable projected trajectory, of the Euclidean/Clifford Lagrangian-based mappable-tracing of the said expansion, — the Flow of the inferred general genus, of such an escalating Lagrangian of Euclidean/Clifford Expansion, as taken through the coni-point, of the proximal locus of the inferred mapped-out semi-set locus, of such an isotropic “spur,” will consequently tend to work to bear the manner, of being of a hermitian nature. However; when one is to have a given arbitrary escalating Lagrangian of Euclidean/Clifford Expansion, that is here to work to bear a mappable isotropically Unstable “spur,” at a semi-set virtually Laplacian-related locus, as this is here to be mapped-out, along the path of the inferred determinable projected trajectory, of the Euclidean/Clifford Lagrangian-based mappable-tracing of the said expansion, — the Flow of the inferred general genus, of such an escalating Lagrangian of Euclidean/Clifford Expansion, as taken through the coni-point, of the proximal locus of the inferred mapped-out semi-set virtually Laplacian-based non-isotropic “spur,” will then consequently tend to work to bear the nature, of working to bear the general condition, of exhibiting a Lagrangian-based Chern-Simons singularity. SAM.

The i*PI(del) Action And Charge

 When a mass-bearing superstring of discrete energy permittivity, is to alter in its motion in relation to electromagnetic energy, the proximal local i*PI(del) Action is to be eminent. Mass-Bearing discrete energy, tends to come in groups, that may thought of here as being mass-bearing cohesive sets of discrete energy quanta. The net composite eminent i*PI(del) Action of a cohesive set of discrete energy quanta, tends to facilitate at working to form a net holonomic substrate of Cohomology-related topological stratum, that  is here to tend to interact with its immediately external environment, over the course of a successive series of group-related instantons, in so as to work to facilitate in the formation, of what may be thought of as being the general phenomenology of charge. I will continue with the suspense later! Sincerely, SAM ROACH.

Some Stuff As To Photons

 Photons just about Never make a “head-on” collision with one another. Or; in other words, an individually taken photon very rarely makes a “head-on” collision with another individually taken photon. The Suspense Is To Be Continued Later! Sincerely, SAMUEL DAVID ROACH. (1989).

Cohesive Riemann-Related Scattering — Homeomorphic Field

 Often when one is to have multiple sets of discrete energy quanta, that are here to interactively engage in the physical exhibition, of a cohesive tense of a Riemann-related scattering, — the resultant field, that is thereby to be subsequently distributed from among the spatial eigenstates, that are of such a covariant tense of an implied interactive display, of sets of discrete energy quanta, will consequently tend to work to bear the sub-tension of a homeomorphic spatial delineation, over the correlative duration, in which such an inferred general genus of a Riemann-related scattering, is thence to occur. To Be Continued! Sincerely, Sam Roach.

Cohesive Rayleigh Scattering — Heterogeneous Morphological Field

Let us say, one were to have multiple sets of discrete energy quanta, that were here to work to bear the exhibition of a cohesive tense of a Rayleigh scattering. The resultant morphology of the covariant field, that would thence be proximal local in its spatial distribution, as this is here to be considered to be taken, amongst the earlier inferred interactive multiple sets of discrete energy quanta — would thereby consequently tend to work to bear a heterogeneous tense of a subtended delineation. HAPPY HOLIDAYS! TO BE CONTINUED! SAM ROACH. (PHS 1989).

Yukawa To The Kahler-Metric — Gliosis Or Not

 Let us initially consider two different yet distinct mass-bearing cohesive sets of discrete energy quanta, that are both here, to act as being Yukawa to the Kahler-Metric. Let us next consider, in this particular case scenario, that both of such discrete sets of energy quanta, are here to each work to bear a mathematically configured mappable-tracing of cohomology-related index, to where the holonomic substrate of the mathematically determined cohomology, may be described at a given arbitrary Laplacian-based locus, when one is to work to mathematically determine, what the thence proximal local latent eigenstate of cohomology is to be — at the inferred given arbitrary Laplacian-related locus. Now, temporarily to go back to a little bit “before”; Both of such inferred sets of discrete energy, are to basically be behaving in the same manner, except that one of these two said cohesive sets of discrete energy quanta, is here to act as being Gliosis to the Kahler-Metric, whereas, the other of these two said cohesive sets of discrete energy quanta, is here to Not act as being Gliosis to the Kahler-Metric. That said set of discrete energy quanta, of the two — that is here to act as being GLIOSIS to the Kahler-Metric — will consequently Tend to result in working to display a deeper scalar amplitude of a Kahler-based quotient, than the other said set of discrete energy quanta, — that is here to Not act, as being Gliosis to the Kathler-Metric. This tendency, is in so long as that the motion of both of these two mentioned mass-bearing cohesive sets of discrete energy quanta, are to simultaneously be occurring, (via the “perspective” of a central coni-point), over a relatively transient duration of discrete time, via the course of an evenly-gauged Hamiltonian eigen-metric. Sincerely, SAMUEL ROACH. (1989).

Diffeomorphic Fields Of Exactly The Opposite Charge

 When one is to have a harmonic pulse, that is here to be subtended in its delineation, between and amongst two different but distinct covariant diffeomorphic fields, that work to bear anti-chiral charges, that are of the same absolute value of scalar magnitude, (that is to say, this is to be appertaining to two different but distinct fields, that are here to work to bear Exactly the opposite charge), this will often tend to consequently result, in the formation of a “cyclically homeomorphic” tense of a flow, in that general classification of those inferred Schwinger-Indices, that are here to be crucial, in the general processes of the transference of the vibrational propagation of the correlative indices of “force.” SAMUEL ROACH.

A Charged Diffeomorphic Field

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

Homeomorphic Field Of Force

 When the covariant field of correlative force, that is here to be kinematically delineated between two or more interdependent interactive discrete quanta of energy, is to be of a harmonic nature, --  the manifold-related topological substrate of the directly corresponding cohesive set of Rarita Structure eigenstates, that are here to be in conjunction amongst these said interdependent interactive discrete quanta of energy, will consequently tend to work to bear, what basically amounts to what is here to act as a homeomorphic field, as this is here to be approximated, over a relatively transient duration of time. TO BE CONTINUED! SINCERELY, SAM.

Some Ideas As To The Collective Consciousness

 The harmonic interactive kinematic multiplicity of centralized thought wave interaction, as this is here to be mapped-out, in a Fourier-related manner, along the arena of space-time-related nodal indices, -- is directly involved with the general gist, as to the basic means, of the general functional operation of the collective consciousness.  I will continue with the suspense later! Sincerely,  SAMUEL DAVID ROACH.

Kinematic Transfer Of Mass-Bearing Phenomenology

 The kinematic transfer of mass-bearing discrete energy quanta, occurs primarily, due to that general contingent tugging of the Lagrangian-related motion, that is of a potentially various genre of open-looped/open-strand phenomenology, that is here to be impelled in an eminent manner, upon such so-stated mass-bearing discrete energy quanta; to where the general type of phenomenology that is here to bear the work of the just mentioned contingent tugging, is here to act as a tense of a Legendre homology, that is thence to be of the essence, of  acting as a general tense of a superstring-related phenomenology, that is of the nature of being discrete kinetic energy quanta. I WILL CONTINUE WIIH THE SUSPENSE LATER! TO BE CONTINUED! Sincerely, SAMUEL ROACH. (1989).

Inertia — Symplectic Geometry Versus Khovanov Geometry

 Superstrings of discrete energy permittivity, that are to work to bear a symplectic geometry, tend to exhibit more of an innate tense of inertia, Than superstrings of discrete energy permittivity, that are, instead, to work to bear a Khovanov geometry. To Be Continued! Sincerely, SAMUEL DAVID ROACH. 

As To Tense Of Inertia — Just A Thought

 The following is just a “thought,” as to a key difference that I perceive — as to a relationship between the general tendency of an abelian light-cone-gauge topology, And, the general tendency of a non abelian light-cone-gauge topology. The general stratum of an abelian light-cone-gauge topology (Kaluza-Klein), tends to be inclined to propagate (phenomenology) Into a general tense of inertia; whereas, the general stratum of a non-abelian light-cone-gauge topology (Yang-Mills), tends to be inclined to propagate (phenomenology) Out of a general tense of inertia. (1989). To Be Continued! Sincerely, SAMUEL DAVID ROACH.

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.

Electromagnetic Energy — Anti-Holomorphic Kahler Conditions

When a given arbitrary superstring of discrete electromagnetic energy permittivity, is to scatter upon the topological manifold of a physical phenomenology, that is here to be considered at a level that is Poincare to the directly associated field density, that is here to be proximal local to the core region, at which the inferred photon, that is in the process of being scattered, is here to be initiating the general process of a Gliosis-related contact, via which the ensuing process of the respective scattering of a discrete increment of electromagnetic energy permittivity, is thence to be brought into the condition of occurring, — this will thereby work to consequently allow for the resultant physical tendency, as taken at the proximal local region of the stated electromagnetic scattering, of a given arbitrary respective set of anti-holomorphic Kahler conditions, that are thence to be present, over the course of the general process, by which the said photon that is here to be in the process of scattering, is thereby to eminently bear the physical condition, of working to bear a tense of a Lagrangian-related Chern-Simons singularity — at the proximal locus, at which the process of scattering is specifically to occur. To Be Continued! Sincerely, SAM ROACH. 

Part Two As To Metrical Pulsation

 As the Polyakov Action is here to be occurring, in an inverse relationship to the general activity of the  the Lorentz-Four-Contraction, — those individually taken superstrings of discrete energy permittivity, that are here to work to bear an even tense, of what is here to be a smooth change in the linear-based increase/decrease, in the scalar amount of the directly applicable Lorentz-Four-Contraction, are to consequently take-hold upon the directly correlative decrease/increase, in the scalar amount of the directly applicable Polyakov Action; — this is thereby to consequently tend to result in occurring in such a manner, to where those mentioned strings of discrete energy permittivity, that are here to be accelerating/decelerating, at an even rate (as a smooth change in the scalar magnitude of the correlative velocity, of which is here to not involve any spurious fluctuations in either the directly corresponding changes in rate And/Or in the absolute value of the directly corresponding Riemann-related directional “heading”) — as this is here to be occurring, over a discrete duration, of which is here to be translated over an evenly-gauged Hamiltonian eigen-metric.  If such a general type of an activity is here to be occurring, via a path wise translation of a spatial transference, that is here to be divvied-out  over the course of a unitary Lagrangian, that is here to be conveyed in a manner, that is piece-wise continuous in its cohomology-related mappable-tracing, then, such a resultant “reverberation” in rate, that is here to consequently occur (to be going “back-and-forth” in pulsation, from a smooth increase in relativistic speed, to a smooth decrease in relativistic speed); — and also, —  then, although such a general tense of motion will consequently tend to be cyclical, in the alteration of its dimensional related pulsation, to where there will thereby be a cyclical durational tense, of the proximal local presence of metric-related Chern-Simons singularities, that will consequently tend to be exhibited here, — the Lagrangian-related aspect of the conveyance of the cohesive set of discrete energy quanta, of which the inferred set of individually taken superstrings that have been mentioned here, are to be acting in so as to work to comprise, as these are here to be transferred through time and space, in a manner that may said to work to allow for that cohesive set of discrete energy quanta that these work to comprise, to bear a hermitian flow in its Lagrangian-related spatial translation, will, however, thereby tend to bear no Lagrangian-related Chern-Simons singularities. This general phenomenology may thereby be described of,  as being the general case, of a smooth Ward-Cauchy-related phenomenology, that is here to be cyclical in its alteration of metrical pulsation. To Be Continued! Sincerely, SAM ROACH. (1989).

As To Fractal Of Flow Towards Cotangent Bundle

 The general flow of mini-string-related segmentation, towards the cotangent bundle, that is here to be directly associated with the proximal local presence, of a given arbitrary cohesive set of discrete energy quanta, — tends to work to bear the fractal of a mappable tracing, as to the general flow of mini-string-related segmentation, towards the cotangent bundle, that is here to be directly associated with the proximal local presence, of those individually taken superstrings of discrete energy permittivity, that work to comprise the initially stated cohesive set of discrete energy quanta. To Be Continued! (1989). Sincerely, SAM ROACH.

Yau-Exact Nature — Forward-Time Momenta

 Mass-Bearing cohesive sets of discrete energy quanta, that are here to be of a Yau-Exact nature — , tend to be comprised of by superstrings of discrete energy permittivity, that are of the general panoply of a forward-time-related momenta. I will continue with the suspense later! To Be Continued! SAM ROACH.

Orientable Superstrings — Yau-Exact Nature

 A mass-bearing cohesive set of discrete energy quanta, is definitively more likely to be of a Yau-Exact nature, if those superstrings of discrete energy permittivity — that work to comprise such a said mass-bearing cohesive set of discrete energy quanta — are of an orientable nature. I will continue with the suspense later! To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

Yau-Exact — Noether Flow

 Mass-Bearing cohesive sets of discrete energy quanta, that are here to be kinematically translated, in a manner that is of a Noether-Flow-related nature, — are definitively more likely to work to bear the general tendency, of acting in a Yau-Exact manner, than those mass-bearing cohesive sets of discrete energy quanta, that are here to be translated, in way that is of a tachyon-related nature. To Be Continued! Sincerely, SAM ROACH.

Heuristic calabi-yau Spaces

 Let us initially consider a given arbitrary mass-bearing cohesive set of discrete energy quanta. The more that the topological manifold, that is here to act as the spatial stratum, of such an inferred type of a set of discrete energy quanta, is to exhibit the Ward-Cauchy-related condition, of working to bear a flat Ricci curvature, — the more likely that those superstrings of discrete energy permittivity, that are here to work to physically comprise the fabric-related composition, of such a said cohesive set of discrete energy quanta, are to heuristically exhibit the general physical characteristic, of behaving as a calabi-yau space. (1989). SAMUEL ROACH.

A Very Special Analogy

 Here’s my take — as to a certain very special analogy (metaphor), that I have “drawn-out” — as to a symbolic relationship that I have considered, as being in comparison between certain general workings in the superstring-related realm, in a correlation to certain general workings in the biological realm.:

The general functional workings, of what I call the superstring-related “Klein Bottle,” when this is here to be in reference to the eminent general superstring-related activity, that is happen, when a given arbitrary cohesive set of discrete energy quanta are to behave, as acting Gliosis to the Kahler-Metric (which is when the multiplicity of certain fractals of discrete energy are re-attained, in a respective correlative manner, in so as to help to work to allow for discrete energy to remain as discrete energy) is metaphorical to discrete energy in the realm of substrings, — what mitochondria, which help to work to allow for an adequate generation of chemical energy (ATP) in animal cells, are, to the perpetuation of the existence of that physical energy, which is needed in a multiplicity of biological life forms — as this is here to be taken, as an analogy between the superstring-related realm AND the biological realm. To Be Continued! Sincerely, SAMUEL DAVID ROACH. (1989).

Floer-Homology, And Gliosis To The Kahler-Metric

 Let us initially consider two different mass-bearing cohesive sets of discrete energy quanta, that are here to be gyrating — over the metric span of a rotational closed circuitry. One of such cohesive sets of discrete energy, is to be transferred at a vantage-point of a reference-frame, that is here to be external from the  Poincare level of the kinematic proximal local covariant mappable locus, that is here to be of the said cohesive set of energy, via the general kinetic processes of a Floer-Homology; whereas, the other of such cohesive sets of discrete energy, is to be transferred at a vantage-point of a reference-frame, that is here to be external from the Poincare level of the kinematic proximal local covariant mappable locus, of the said cohesive set fo energy, via the general kinetic processes of a homology-related topological manifold, that is Not of the nature of acting as a Floer-homology. Otherwise; the two different and distinct said sets of energy, are here to behave in pretty-much the same general type of a manner. That mass-bearing cohesive set of discrete energy quanta, that is here to be externally transported in a kinetic manner, over a correlative duration of a discrete amount of time —via the general processes of a Floer-homology, will tend to bear a greater tendency of acting as being Gliosis to the Kahler-Metric — than that other mentioned (inferred) mass-bearing cohesive set of discrete energy quanta, that is, instead, to be transported in such a manner, that is here to Not be done, via the general processes of a Floer-Homology. To Be Continued! Sincerely, SAM ROACH. (1989.)

The “Work” Of Partitions

 One may perceive the i*PI(del) Action, as being the “work” of the exchange of superstring-related partition-based discrepancies — when this is to be considered, in terms of both the scalar amount of such discrepancies, that are here to be present, from within the Ward-Neumann bounds of the core-field-density, that is of any given arbitrary distinct superstring of discrete energy permittivity (or, as well — yet in an asymmetric manner in relation to that of its respective superstring, from within the Ward-Neumann bounds of the core-field-density, of any given arbitrary correlative counter string), and/or as well, as such an inferred situation is to potentially vary in the delineation of such stated/inferred partition-based discrepancies. SAM ROACH.

Part One — As To Metrical Pulsation

 Let us initially consider a distinct given arbitrary superstring of discrete energy permittivity, that is here to be perturbative, over a set of a metrical-based sequential series of instantons, — when in terms of the scalar magnitude of its directly corresponding Lorentz-Four-Contractions, that are acting in a Gliosis-based manner, at the Poincare level to the topological surface of the holonomic substrate of the so-stated superstring of discrete energy permittivity, over the span of a proscribed discrete increment of time.  Let us next consider, that those said superstrings of discrete energy permittivity, that are here to be differentiating in a Fourier-related manner, through a given arbitrary Hamiltonian operand — that is here to span the space, by which the so-stated superstring of Hamiltonian-related operation, is to be pulled, in a kinematic manner, through the set path, that is correlative to its directly corresponding discrete Lagrangian, by which the so-inferred eigenstate of discrete energy per cohomology-related generation, is to ensue, in so as to be brought into a reverse-fractal-related interaction, with its correlative externalized attribute of energy per charge (voltage), — as this is here to work to involve, taking the correlative attribute, as taken at an internal reference-frame, of Lagrangian wave-tug at instanton, per cohomology-related generation — while then, perceiving this sort of a behavior at a more external reference-frame, — in order to be able to consider the general physical condition of energy per charge. Let us say, now, that the tense of the directly appertaining perturbation of the correlative Lorentz-Four-Contractions, that are here to be directly applied to the correlative Polyakov-based mechanism, in a kinematic manner — whereby the so-stated discrete quantum of energy permittivity, is to be of a harmonic-related cyclical manner, — that would here work to form an even tense of a gradual increase in the directly applicable amplitude of the quantum effect, as to how an acceleration/deceleration of such a general respective type of a phenomenology, as this is here to be taken, via the motion of a unitary Lagrangian (via a metric, that is here to be transferred — via the kinematic translation of a phenomenon, that is here to be mappable, via a projected path, that is here to be taken via a unitary transversal direction), to where this is therefore to work to effect the gradual alteration, in either both the scalar magnitude and/or in the delineation of the directly applicable Lorentz-Four-Contractions, to where, such a general genus of a type of an activity in the sub string-related realm, will consequently tend to work to bear the Inverse of the effect, as to the proximal local presence, (which, in other words, is here to be of a corollary-based effect), upon the gradual alteration, in either both the scalar magnitude and/or in the delineation of the directly applicable Polyakov Action. ... To Be Continued! Sincerely, SAM ROACH.

Affinity For Exhibiting Anti-Gravity

 Mass-Bearing phenomenology, that are eminently comprised of, by highly magnetic cohesive sets of discrete energy quanta, that are here to work to bear a recurrent tendency of being Gliosis to the Kahler-Metric, — tend to bear a relatively higher affinity, of being able to bear a greater capacity of exhibiting the characteristics of anti-gravity, than other equally magnetic mass-bearing phenomenology, that are not to tend to be able to bear as much of a recurrent tendency, of being Gliosis to the Kahler-Metric. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Anti-Holomorphic Gyration

 The anti-holomorphic-related gyration of mass-bearing cohesive sets of discrete energy quanta, (that are here to bear the tendency, of having a relatively strong tense of a Majorana-Weyl-Invariant-Mode), often tend(s) to work to facilitate the ensuing formation, of the presence of anti-gravity. Sincerely, SAM ROACH.

Anti-Holomorphic Kahler Conditions — Anti-Gravity

 The more recurrently that a given arbitrary cohesive set of discrete energy quanta, is to work to bear the general physical attribute of Anti-Holomorphic Kahler conditions —  the more likely that such a said cohesive set of discrete energy quanta, will consequently tend to display an aptitude, for responding effectually, to the proximal local presence of an applied force of anti-gravity. Sincerely, SAM ROACH.

Nijenhuis Versus Ward Polarization

 The general difference between what I mean by a “Nijenhuis-Polarization” and a “Ward-Polarization,” is that what I call a Nijenhuis-Polarization, is only to be that general tense of a Ward-Polarization — that is to be occurring, over the course of a given arbitrary Fourier-Transformation; whereas, a Ward-Polarization — may be in consideration, over the general course of either a Laplacian Transformation, Or, over a Fourier Transformation. SAM ROACH.

More As To Nijenhuis Polarization

 When two different and distinct phenomenology, that are here to work to bear a spatial transference, that is to be conducted along the Hamiltonian Operand, of each of their respective individually taken Ward-Supplemental Lagrangian-based paths, are thence to work to bear the general physical condition, of being orthogonal to one another, in an Imaginary manner (due to a general covariant Nijenhuis physical condition), to where the holonomic substrate of each of these two different and distinct said phenomenology, are to result in ending-up colliding with each other in a Gliosis-related manner, — then this general resultant type of a Yukawa-related contact, will consequently often tend to result, in a path-wise perturbation in the Fourier-related translation, of both of their individually taken respective Lagrangian-based field operators, to where this tense of a Ward-Cauchy-related gauged action, will thereby often tend to work to allow for the reductional physical condition, of what I term of as being, a state of “Nijenhuis Polarization.” I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989).

Ward-Supplemental Perturbation

 The more recurrently that the Lagrangian-based path of a cohesive set of discrete energy quanta, is to work to bear a Ward-Supplemental perturbation in its delineation, over a respective proscribed duration of time (which is here to be considered, over a respective proscribed sequential series of group-related instantons), the more likely that such a said set of discrete energy quanta, will consequently tend to work to bear the general attribute, of exhibiting the proximal local characteristics, of what may here be thought of as being the presence of Anti-holomorphic Kahler conditions. The more recurrent that a set of discrete energy quanta, is to work to exhibit Anti-holomorphic Kahler conditions, the more likely that such a said set of discrete energy quanta, will then have a greater tendency of being more Gliosis to the Kahler-Metric. Therefore; the more recurrently that the Lagrangian-based path of a cohesive set of discrete energy quanta, is to work to bear a Ward-Supplemental perturbation in its delineation, over a Respective proscribed duration of time (which is here to be considered, over a respective proscribed sequential series of group-related instantons), the more likely that such a said set of discrete energy quanta, will consequently tend to work to bear the general attribute, of acting as being Gliosis to the Kahler-Metric. SAM ROACH. (1989).

Path Of Tendency Of Various Phenomenology

 Light tends to travel, in the directional path of least time. 

Kinetic energy tends to travel, in the directional path of least order.

Noether-based mass tends to travel, in the directional path of least Real Riemannian resistance.

Tachyon-related mass tends to travel, in the directional path of least Nijenhuis (Imaginary) resistance. 

SAM ROACH. (1989).

Number Of Dimensions Of Cyclical Spin — Kaeler-Metric

 Let us consider two different mass-bearing cohesive sets of discrete energy quanta, that are here to each be orbiting around the surface of two similar yet uniquely different closed-looped topological manifolds, in a covariant manner, as this is here to be considered, to be taken over the relativistic span, of the same overall duration of time — via the “perspective” of a central coni-point. One of these two sets of cohesive energy, is to work to bear a cyclical rotation (spin), around a closed-looped circuitry — in one number of spatial dimensions; whereas, the other one of these two different sets of cohesive energy, is also to work to bear a cyclical rotation (spin), around a closed-looped circuitry — in a higher number of spatial dimensions, than the other one of such cohesive sets of discrete energy quanta. That mass-bearing cohesive set of discrete energy quanta, which is here to be rotating around a closed-looped circuitry, that is of a higher number of spatial dimensions, than the other one of the two said sets of cohesive energy, will consequently tend to work to bear a greater tendency of being Gliosis to the Kaeler-Metric, than the other one of these two said sets of discrete energy. I will continue with the suspense later! To Be Continued! (SAM ROACH).

Electrons, Wick Action Eigenstates, And Landau-Ginzburg Eigenstates

 Since those cohesive sets of discrete energy quanta, that work to comprise the physical structure of electrons, tend to exhibit a greater nature, of acting as being Gliosis to the Kaeler-Metric, electrons are consequently, to tend to exhibit the generation, of a larger number of both Wick Action eigenstates And Landau-Ginsburg (Action) eigenstates, over any set period of time, than their directly correlative (respective) nucleons do. I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989). 

Electrons — As To Being Gliosis To The Kahler-Metric

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

Isotropic Stability And The Kahler-Metric

 The more isotropic stability, that a given arbitrary charged mass-bearing cohesive set of discrete energy quanta, is to work to exhibit, over a proscribed given arbitrary duration of time, — as such an inferred set of discrete energy, is here to be Gliosis to the Kahler-Metric — the more likely that such a general genus of a said cohesive set of discrete energy, will consequently tend to retain its given arbitrary externalized net scalar amplitude of magnetism — as this is to be taken over a duration, which is here to be considered, over the course of a given arbitrary evenly-gauged Hamiltonian eigen-metric. SAMUEL ROACH.(1989).

Thrust Of Externalized Angular Momentum

 When a harmonic torque is to be applied, to a given arbitrary kinematic charged mass-bearing cohesive set of discrete energy quanta, this general type of an action, will consequently tend to Increase the resonant mobility of the general thrust, that is of its externalized angular momentum; however, when an anharmonic torque is to be applied, to a given arbitrary charged kinematic mass-bearing cohesive set of discrete energy quanta, this general type of an action, will consequently tend to Decrease the resonant mobility of the general thrust, that is of its externalized angular momentum. SAMUEL DAVID ROACH. (PHS 1989).

Gliosis To The Kahler-Metric — Overcoming The Covariant Proximal Local Gravity

 The more that a mass-bearing cohesive set of discrete energy quanta, is to work to bear the general characteristic of being Gliosis to the Kahler-Metric, the more likely that such a said mass-bearing cohesive set of discrete energy quanta, is to be able to bear a higher probability, — of overcoming that impedance, which is of the otherwise inhibiting covariant proximal local force of  gravity. Sincerely, SAM ROACH.

Some Stuff As To Being Gliosis ToThe Kahler-Metric

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

Permittivity/Impedance — Substring-Related Tense Of A Fractal Of Momentum

 The multiplicity of the general “spur” of substring-related sub-cohomology, happens to exhibit a general wave-tug, that is to tend to reverse-fractal, into working to bear the eminent qualities, of a general manner of angular momentum. Furthermore; the multiplicity of the general “settling” of substring-related sub-cohomology, happens to exhibit a general wave-tug, that is to tend to reverse-fractal, into working to bear the eminent qualities, of a general manner of spin-orbital momentum. To Be Continued. Sincerely, SAMUEL DAVID ROACH.

Rate Of Cycling Through Anti-Holomorphic Kahler Conditions, And Magnetism

 Let us consider the general activity, of a mass-bearing cohesive set of discrete energy quanta. The quicker that such a said set of discrete energy quanta, is to cycle through the general process, of working to bear the general characteristic, of having an attributable set of Anti-Holomorphic Kahler Conditions, as appertaining to the properties of its co-determinable action, the quicker that such a said set of discrete energy quanta, will consequently tend to bear a perturbation, in its directly corresponding Chern-Simons Invariants. (Which are only “invariant,” when the motion of such a said set of cohesive energy, is to maintain the same tense of motion, in its relation to “light.”) Therefore; the quicker that such a said set of discrete energy quanta, is to cycle through the general process, of working to bear the general characteristic, of having an attributable set of Anti-Holomorphic Kahler Conditions, as appertaining to the properties of its co-determinable action, the more magnetism that such a said mass-bearing cohesive set of discrete energy quanta, will thereby tend to generate — as this is here to be taken under the covariant stipulation, of considering this to be happening, over the same comparative duration, of a common span of an evenly-gauged Hamiltonian eigen-metric. To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Greater Scalar Magnitude Of Magnetic Generation — Due To Rotational Cycling

 Let us say, one were to have a situation, to where there were to be two different case scenarios — that were each to work to bear the general condition, of two different relatively macroscopic tenses of electrical cycling, by which, each of such individually taken case scenarios, were to work to involve the motion of one distinct electron, per each so-inferred individually taken case. Each of these electrons, was to be moving at Exactly the same covariant-related rate of speed — in its relation to the motion of electromagnetic energy. This is to where — one is to have a situation, to where one of such electrical cyclings, works to involve an electron, that is to simply be reverberating in a back-and-forth manner (via the distance of one meter of length, back-and-forth); whereas, in the other given case scenario, the electron is to be orbiting in its path, in a relatively circular manner (in which the circumference of the herein inferred cyclical path, is to incur a spatial distance of one meter). Since the electrical cycling — that is here to be of an orbital nature — is to be altering more often in its direction, in its relation to the motion of electromagnetic energy, such a said tense of electrical cycling, will consequently tend to bear a greater scalar amplitude of a perturbation in its Chern-Simons Invariants, when this is here to be taken over the conditions, of a time-related piece-wise continuous function. (Please keep in mind, again, that Chern-Simons Invariants are only “Invariant,” when both the rate, as well as the direction, of a cohesive set of discrete energy quanta, is to stay the same, in its relation to electromagnetic energy.) This just mentioned tendency, will consequently tend to result, — in the general condition, — by which the Circular tense of electrical cycling, will thereby tend to bear a greater tense of a net magnetic generation, than the other tense of electron cycling will. SAM.

Discrete Energy Quanta

 The multiplicity of the Ward-Cauchy-related holonomic metric-gauging, that is of the nature of a tense of a holomorphic wave-tug, via its behavior as an eigenstate, of the nodal disturbance of the general pressurized vacuum, that is of the realm of space-time-fabric, acts as the demonstrable source of causality — that works to function, as the operational entity of the general exhibition of discrete energy quanta. The “spur” of such inferred discrete energy quanta, tends to act as the phenomenology of superstrings of discrete energy permittivity; while the “settling” of such inferred discrete energy quanta, tends to act as the phenomenology of discrete energy impedance. SAM ROACH. I will continue with the suspense later!

Group-Attractors/“Ghost”-Based Inhibitors

 The so-called “resistivity” of sub-cohomology-related eigenstates, may tend to basically be described of as being, the general entity, of what I call “ghost-based inhibitors.” Furthermore; the so-called “conductivity” of sub-cohomology-related eigenstates, may tend to basically be described of as being, the general entity, of what I call “group-attractors.” To Be Continued! Sincerely, SAM ROACH. (PHS1989).

A Little Bit About Resistivity And Conductivity

 The “resistivity” of the myriad exhibition of sub-cohomology eigenstates, tends to help at working to reverse-fractal — into the general physical condition of impedance. Furthermore; the “conductivity” of the myriad exhibition of sub-cohomology eigenstates, tends to help at working to reverse-fractal — into the general physical condition of permittivity. I will continue with the suspense later! Sincerely, SAMUEL.

Part Of What Works to Bring About The Need For The i*PI(del) Action

 When a given arbitrary cohesive set of sub-cohomology eigenstates, are to work to bear the general action, of a respective inverted coupling (or, in other words, to where these said eigenstates, are to work to bear the general action of a Decoupling) with a discrete quantum of zero-point-energy, — this general process, Indirectly works to bring about the need, for the existence of the i*PI(del) Action. Sincerely, SAM ROACH.

Coupling “Series” Of “Cyclic Permutation”

 Here’s my take, as to how one may be able to attempt to calculate — the general scalar magnitude, of an eigenstate of a Sub-Cohomology-related “topological manifold.” : 

1) Initially, consider the following Coupling “Series” Of “Cyclic Permutation.”;

[{OF N=1}((((e^(((e^((i!)*(N/2)))*(1/N)))/e^(((-i)!*(N/2))^(-1))) * {OF N=2}((((e^(((e^((i!)*((N(1)+1)/2)))*((1/(N(1)+1)))/e^(((-i)*((N(1)+1)/2))^(-1))) * {OF N=3}... [UP TO THE Integer Number Of The Directly Corresponding Beti Number, {This is to where, “N” is the absolute value of the directly corresponding Beti Number}]]  Multiplied By [The directly corresponding value, that is here to be directly corresponding to The i*PI(del) Action {To Where, if one is here to be dealing with only one discrete increment of the i*PI(del) Action, one will here be applying the value of “8.635858*10^(-63) Coulombs-Seconds}] Multiplied By [The Lagrangian Of The correlative Zero-Point-Energy{ Or, in other words, as multiplied ty the value of (-i)* the scalar magnitude of the correlative zero-point-energy, as in terms of Joules-Seconds}]. This is, at this particular point in explanation, just beginning to describe the general scalar magnitude of sub-cohomology.  In the Real World, one is to also be have the need to couple this math, — with the application of an appropriate given arbitrary path integral. Enough for now! Sincerely, Samuel David Roach. (To Be Continued!) (PHS 1989). P.S.: I apologize if I may have made any errors in the “parentheses.” I’ll check this again tomorrow!

Nijenhuis Polarization

 That general tense of polarization, by which certain genre of gravitational waves — may be converted into various genre of thought waves — is basically of the means of a given arbitrary example, of what I term of as being, a NIJENHUIS POLARIZATION.  (1989). I will continue with the suspense later! Sincerely, SAMUEL ROACH.

Reverse-Fractal Of Super String-Related Permittivity/Permeability

 When a mass-bearing discrete quantum of physical energy, is to work to exhibit a relatively strong tense of permittivity, this general condition will tend to reverse-fractal, into the existence of mass-bearing cohesive sets of discrete energy quanta — that are consequently to result, in tending to Externally display a relatively strong scalar magnitude of charge per time (amperage). Furthermore; when a mass-bearing discrete quantum of physical energy, is to work to exhibit a relatively strong tense of permeability, this general condition will tend to reverse-fractal, into the existence of mass-bearing cohesive sets of discrete energy — that are consequently to result, in tending to Externally display a relatively strong scalar magnitude of energy per charge (voltage). The microscopic condition of  increased “amperage,” may often reverse-fractal into the physical condition, by which a physical entity, at the vantage-point of a much larger scale of measurement, may then tend to work to bear a stronger fractal modulus. Furthermore; the microscopic condition of increased “voltage,” may often reverse-fractal into the physical condition, by which a physical entity, at the vantage-point of a much larger scale of measurement, may then tend to work to bear a stronger elastic modulus. Consequently; a strong tense of super string-related energy permittivity, may often tend to be able to reverse-fractal, in a vast manner, into the presence of a strong tense of fractal modulus. Furthermore; a strong tense of super string-related energy permeability, may often tend to be able to reverse-fractal, in a vast manner, into the presence of a strong tense of elastic modulus. SAM.

Sub-String-Related “Shimmying”

 The more that a super string of discrete energy permittivity, is to “shimmy” from a heuristic Noether-related manner, the more of a “swivel-shaped” contour, that the directly corresponding topological mappable surface of such a string, will consequently tend to be exhibiting. To Be Continued! Sincerely, SAMUEL(1989).

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).

Compensation — Due To Relations, Involving “Regional-Swipe-Inhabitation”

 That physical condition, by which sub-cohomology-related eigenstates, are to tend to work to bear a greater scalar magnitude of a covariant “regional-swipe-inhabitation,” as the spatial dimensionality of the directly corresponding proximal local mass-bearing super string of discrete energy permittivity is to increase in its value, — works, to compensate for the general physical condition — to where, when two of such different inferred Noether-related mass-bearing super strings , that are here to otherwise be of the same basic nature, are to work Alter by a different number of spatial dimensions, — the scalar magnitude of their directly corresponding “regional-swipe-inhabitation,” will consequently tend to result in basically being of the same  scalar magnitude. So; when the Beti number is to increase/decrease (for a super string of discrete energy permittivity, that is to otherwise, besides altering in its number of spatial dimensions, to be of the same general nature), in order for the “regional-swipe-inhabitation” of the correlative super string to be maintained in its scalar magnitude, — the directly corresponding individually taken proximal local eigenstates of sub-cohomology, are to respectively increase/decrease, in their correlative scalar magnitude. I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH.

More As To Inverted Energy-Charge

 The accelerated/decelerated inverted energy-charge of holonomic metric-gauge eigenstates, tend to work at helping to form the general phenomenology, of the multiplicity of the proximal local presence, of the corroborative sub-cohomology eigenstates. The greater that the “regional-swipe-inhabitation” is to be, for those sub-cohomology eigenstates, that are here to be proximal local to a super string-related region, the more that the resultant relationship, that is here to be of that mathematical expression, which is to be signified by the Beti number, is to work to involve a higher integer value, in expressing the stated Beti number. Consequently; the higher that the absolute value of the directly corresponding Beti number is to be, the more change that the spatial dimensionality of the directly corresponding proximal local super string of discrete energy permittivity, is to exhibit. Thank you for reading! SAM ROACH. (PHS1989).

Inverted Energy-Charge

 The proximal local presence of metric-gauge holonomy Per Sub-Cohomology-Related eigenstate, tends to work to form the consequentially accelerated proximal local presence, of a fractal of “inverted energy-charge.”  I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989).

Sub-Cohomology

 Let me soon introduce to you, a new concept that I have been thinking of lately. This concept appertains, to the Ward-Cauchy presence, of a fractal of Cohomology. Just as Cohomology appertains to the “physical memory” of the general interaction, of super strings With point particle-related physical norm-state-projections (such as zero-norm-state-projections, Campbell norm-state-projections, Hausendorf norm-state-projections, And Campbell-Hausendorf norm-state-projections); — That inferred fractal of Cohomology, of which I am to name of here, as being on the order of acting as Sub-Cohomology eigenstates, — may more aptly be described of as being, the “physical memory” of the general interaction, of first-order point particles With zero-point-energy. The higher that the directly corresponding Beti number is to be, — that is here to be directly associated with the metric-related gauging of the spatial dimensionality, of the respective corroborative super strings, — the greater that the scalar magnitude will consequently tend to be, of the proximal local presence, of the directly appertaining Sub-Cohomology eigenstates, that are thence formed. Consequentially; the lower that the directly corresponding Beti number is to be, — that is here to be directly associated with the metric-gauging of the spatial dimensionality of the respective corroborative super strings, — the smaller that the scalar magnitude will consequently tend to be, of the proximal local presence, of the directly appertaining Sub-Cohomology eigenstates, that are thence formed. SAM (1989). 

Reverse-Fractal Into Highly Conductive Phenomenology

 Mass-Bearing Noether-based superstrings of discrete energy permittivity, that bear a strong tense of isotropic stability, have the general tendency, of being able to reverse-fractal towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of magnetism. Furthermore; phenomenology that are to exhibit a high tense of magnetism, tend to reverse-fractal, towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of conductivity. Consequently; mass-bearing Noether-based superstrings of discrete energy permittivity, that bear a strong tense of isotropic stability, often tend to have the general tendency, of being able to reverse-fractal towards the general attribute, of directly associating with phenomenology, that are to work to exhibit a high tense of conductivity. To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Regional Swipe Inhabitation

 Let us say that one were to have two different Noether-based mass-bearing super strings of discrete energy permittivity. Over a given arbitrary Laplacian condition, both of such said strings, are to work to bear the same Lorentz-Four-Contraction; as well as that both of such said strings, are also to work to bear the same general tense of a swivel-like contour. However; one of such super strings of discrete energy permittivity, is to have a higher spatial dimensionality than the other one. Due, in part, to the increase in the tensor-related set of attributes, that are here to be directly corresponding, to the manner by which the correlative partition-based discrepancies, that are here to be appertaining to the string that is exhibiting a higher number of spatial dimensions, is to be delineated — this situation will thereby consequently tend to result, in the general physical Ward-Neumann-related condition, by which both of such said strings, will thereby tend to exhibit basically the same scalar magnitude of “regional-swipe-inhabitation” as each other, — over the thus inferred Laplacian-based physical condition, in which both super strings of discrete energy permittivity, are to be compared, in a manner that is both covariant, co-determinable, and co-differentiable, via the “perspective” of a central coni-point, during the same venue of iteration of the inferred group-related instanton. I will continue with the suspense later! (1989). Sincerely, SAM ROACH.

Operations That A Cohesive Set Of Discrete Energy Quanta May Perform

 A given arbitrary mass-bearing cohesive set of discrete energy quanta, that is gauged in an isotropically stable manner — in so as to exhibit a group action — may perform between one to four different specific “impelling” tasks, over the durational span of a relatively transient sequential series of group-related instantons. (As this is here to be considered to be taken, over an evenly-gauged Hamiltonian eigenmetric.) I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (PHS 1989).

Unilateral Direction-Related Wave-Tug

 Let us initially consider two different tachyon-related mass-bearing cohesive sets of discrete energy quanta. One is to work to bear a Fourier-related gauged-action, that is here to be acting as the holonomic substrate of a monomial group action; whereas, the other implied set of cohesive discrete energy quanta, is to work to bear the Fourier-related gauged-action, that is here to be acting as the holonomic substrate of a quadranomial  group action. That set of discrete energy quanta of the two, that is here to be of the nature of acting as an entity, that is here to be exhibiting the behavior of a monomial group action, will tend to work to bear a tachyon-related Nijenhuis impedance, that is to exhibit a direction-related wave-tug, that is here to be delineated in a Li-antichiral-related manner, when in relation to the directly corresponding spatial translation, that is of the correlative angular momentum eigenstate, that is of its covariant co-differentiation with the correlative adjutant proximal local tachyon-related holomorphic permittivity, that is here to be most directly associated with the innate superstring-related directional “drive,” that is of the proximal local discrete energy permittivity, of such a given arbitrary case scenario. However; that set of discrete energy quanta of the two, that is here to be of the nature of acting as an entity, that is to be exhibiting a quadranomial group action, will tend to work to bear a tachyon-related Nijenhuis impedance, that is to exhibit a direction-related wave-tug, that is here to be delineated in a manner, that is of both a Real Riemannian and of a positively chiral nature, when in relation to the directly corresponding spatial translation of the correlative angular momentum eigenstate, that is of its covariant co-differentiation with the correlative adjutant proximal local tachyon-related holomorphic permittivity, that is here to be most directly associated with the innate superstring-related directional “drive,” that is of the proximal local discrete energy permittivity, of such a given arbitrary case scenario. This consequently tends to work to make the said tachyon-related holomorphic permittivity — that is, in the particular case, of the superstring-related set of discrete energy quanta, that is here to be acting as a quadranomial group action, to consequently tend to result, in working to bear a unilateral direction-related wave-tug, with the directly corresponding metric-gauge eigenstate, that is most proximal local to the eminent spur in the covariant co-differentiation, that is of the kinematic activity of its correlative tachyon-related Nijenhuis impedance. (1989). To Be Continued! Sincerely, SAM ROACH.

Tachyon-Related Nijenhuis Impedance

 When one is to have a mass-bearing cohesive set of discrete energy quanta, that is here to be behaving in a tachyon-related manner, — the more spatial dimensions that such a said set of discrete energy quanta is to be exhibiting, over a set duration of time, the more acute that the angling of its directly corresponding Nijenhuis impedance will tend to be, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass-bearing cohesive set of discrete energy quanta. For example: Let us consider two different cases of such inferred sets of mass-bearing discrete energy quanta. One of such sets is to be of a three spatial dimensional nature, while the other of such sets is to be of a six spatial dimensional nature. Both of such sets of discrete energy quanta, are here to be behaving as tachyons; as well, as that both of such sets of discrete energy quanta, are otherwise to be behaving in basically the same general manner of a covariant spatial translation — over a discrete quantum of relativistic time, — as taken over the vantage-point of a central coni-point, that is here to be translated through space, over an evenly-gauged Hamiltonian eigen-metric. The just mentioned mass-bearing set of discrete energy quanta, that is here to be exhibiting the nature of behaving as a superstring-related entity, involving six spatial dimensions, will consequently tend to bear a smaller subtended angle of a Nijenhuis impedance, that is here to be imparted upon the correlative gauge-action, of the proximal local angular momentum field eigenstate, that is related to the co-differentiable permeability of the said mass- bearing cohesive set of discrete energy quanta. (1989). To Be Continued! Sincerely, Samuel David Roach.  

Centripetal Force And Charged Particle

 Let’s consider a mass-bearing cohesive set of discrete energy quanta, that is to be rotating, via a parabolic path, that is here to also be simultaneously tugged into one specific transversal direction, over a given arbitrary discrete duration of time. Let us now consider, that there is here to be a designated group action, of which is to work to involve a cohesive operation of many individually taken inferred sets of cohesive energy quanta. The greater that the correlative centripetal force, that is here to be applied to an overall set of the multiplicity of a charged mass-bearing cohesive set of discrete energy quanta, over the earlier implied duration of time, the stronger that the angular momentum will tend to be, — as this is here to be taken, in lieu of the implied transversal direction in which such a herein stated set of discrete energy, that is here to be operating to perform one common function, is to be tugged through (upon), to where the just implied act of torsion, will consequently tend to work to increase the resultant aerodynamics of the said overall set of composite individually taken mass-bearing sets of cohesive energy quanta. SAM ROACH.

Magnetism Directly Associated With Charge

 Let us initially consider a charged mass-bearing cohesive set of discrete energy quanta, that is here to be transferred from one given arbitrary locus to another given arbitrary locus. The quicker that the correlative Chern-Simons Invariants are to perturbate, that are here to be of the said respective mass-bearing cohesive set of discrete energy quanta, to where these are here to be most directly associated with the general process of the flow of the charged motion, of such an inferred set of interdependent discrete energy, to where this will consequently tend to reverse-fractal into bearing the result, of such a general kinematic tense of an inferred type of a procedure, of which is here to be directly corresponding to the Lagrangian-based motion of a superstring-related Fourier Transformation of a charged particle, that is being transferred through space over time, to where this particular scenario of a charged mass-bearing cohesive set of discrete energy quanta, is thence to tend to work to bear a heightened scalar amplitude of magnetism associated with its charge, as when compared to an ulterior superstring-related situation, in which the correlative Chern-Simons Invariants are to alter in the exhibition of their delineation in a slower manner, of a covariant-related tense of change over time.To Be Continued! I will continue with the suspense later! Sincerely, Samuel David Roach. (PHS1989).

Nijenhuis Direction Of Magnetic Thrust

 Mass-Bearing cohesive sets of discrete energy quanta, that are here to work to bear a tense of a fractal of magnetic thrust, — that is here to work to bear a Nijenhuis tense of delineation, — tend to have a greater probability of potentially bearing an effect upon phenomenology that is of other universal settings, than other mass-bearing cohesive sets of discrete energy quanta, that are to have the bearings of a fractal of  magnetic thrust, that is instead, to only work to bear a Riemannian tense of delineation. To Be Continued! Sincerely, SAM ROACH.

As To Why Fermions Tend To Have A Greater Charge Density

 One of the reasons — as to why mass-bearing cohesive sets of discrete energy quanta, that operate, in so as to work to bear a fractional spin (super small particles that work to bear a fractional spin, are commonly  named of as being fermions), tend to work to bear a greater charge density, than mass-bearing cohesive sets of discrete energy quanta, that instead, operate, in so as to work to bear a whole spin (super small particles that work to bear a whole spin, are commonly named of as being bosons), — is to basically be of the herein mentioned reason: mass-bearing cohesive sets of discrete energy quanta, that are here to exhibit a fractional spin, — tend to exhibit a more spurious alteration in their Chern-Simons Invariants, during the process in which such a set of particles, that are here to work to bear a fractional spin (the respective fermions), are to alter in their direction and/or in their rate of motion, when this is here to be considered, in their relationship to the motion of electromagnetic energy. To Be Continued! Sincerely, SAM ROACH. (PHS 1989).

Charge Density

 Cohesive sets of discrete energy quanta, that are here to work to bear a fractional spin, tend to reverse-fractal into exhibiting a greater charge density, than cohesive sets of discrete energy quanta, that are, instead, to work to bear a whole spin. To Be Continued Later! Sincerely, Samuel David Roach. (PHS,1989).

Magnetic-Related Thrust

 The more that a given arbitrary mass-bearing cohesive set of discrete energy quanta, is capable of tending  to be able to exhibit a greater attribute of tensor-related metric displacement over time, — the more that such a said respective mass-bearing cohesive set of discrete energy quanta, is thence to consequently tend  to be capable of achieving a greater magnetic-related thrust in the process. To Be Continued! SAM ROACH.

Affinity To Responding To Anti Gravity

 The higher that the Kahler-based quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, the greater that the directly corresponding Majorana-Weyl-Invariant is consequently to tend to be.  The greater that the correlative Majorana-Weyl-Invariant mode is to be, the deeper that the directly corresponding resonant vibration, that the respective given arbitrary mass-bearing cohesive set of discrete energy quanta, is consequently to tend to be. The deeper that the correlative resonant vibration is to be — when this is here to be taken in terms of the respective directly corresponding mass-bearing cohesive set of discrete energy quanta, the more that such a herein stated set of discrete energy quanta, is consequentially to have a stronger affinity of responding in an effectual manner, to the proximal local presence of anti gravity. Therefore; the higher that the Kahler-based quotient is to be, for a given arbitrary respective mass-bearing cohesive set of discrete energy quanta, the greater that such an inferred  discrete set of inter-related energy quanta, that are here to be operating, in so as to perform a group-related function over time, will consequently tend to result, in working to bear a greater affinity of responding in an effectual manner, to the proximal local presence of anti gravity. To Be Continued! Sincerely, SAM ROACH.

Some Potentially Viable Thoughts AsTo Cohomology-Related Eisenstate Of An F-Field

 Here is a mathematical idea, as to my present perception is to be, in regards to how to help in describing — what the cohomology-related eigenstate of an f-field is:

Initially; take the knotting equation, for whatever the dimensionality of the given arbitrary respective cotangent bundle, for what the directly associated field is to be — as this is here to be taken, in terms of “gamma-knot” — while then multiplying this by the mathematical expression for the product of the Planck Constant, as this is here to be coupled with the applicable square of the directly associated discrete increment of time. Next; Divide this whole just mentioned or inferred expression, by the following, — Take the value of “8*PI^2.”  Multiply this by the following type of a general series of Hamiltonian Operators — ((The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by the square-root of two) + (The Square of The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by two) + (The Cube of The Hamiltonian Operator that is most associated with the correlative respective Knot Divided by two times the square-root of two) + (The Fourth Power of the Hamiltonian Operator that is most associated with the correlative respective Knot Divided by four)).  The consequential resultant of this just inferred mathematical process, is what I perceive to be, as a means of working to describe the entity of a cohomology-related eigenstate. Please feel free to indicate to me, whether or not this idea is reasonably decent! Sincerely, SAM ROACH.

Proximal Local Presence Of Kahler-based Quotients

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

Legendre Homology And De Rham Cohomology

 Let us consider two different scenarios, of conveyed discrete mass-bearing energy quanta. One of such respective given arbitrary “scenarios,” is to work to bear a tense of a directly corresponding mass-bearing cohesive set of discrete energy quanta, of which is to be conveyed by an isotropically stable Legendre (co)homology; whereas, the other inferred respective given arbitrary “scenario,” is to work to bear a directly corresponding mass-bearing cohesive set of discrete energy quanta, of which is to be conveyed by an isotropically unstable Legendre (co)homology. Otherwise, both of these two scenarios, as to the conveyance of a set of mass-bearing discrete energy quanta, — are basically of the same nature. That given respective scenario of the two, that is to involve a mass-bearing cohesive set of discrete energy quanta — that is here to involve its directly corresponding conveyance, via the kinematic spatial translation of an isotropically stable Legendre (co)homology, via a correlative Fourier Transformation, will consequently tend to have a greater probability of working to involve a resultant De Rham cohomology, than the other given respective case scenario, — of which is here, instead, to tend to have a greater probability of working to involve its conveyance of a mass-bearing cohesive set of discrete energy quanta, via the kinematic spatial translation of an isotropically unstable Legendre (co)homology — in so as to be more likely to tend to work to form a Dubeault cohomology . TO BE CONTINUED! Sincerely, SAMUEL DAVID ROACH. (1989)!

Tense of Legendre Homology

 Let us initially consider two different tenses, of the conveyance of a mass-bearing cohesive set of discrete energy quanta. Let us say, that both of the two different mass-bearing cohesive sets of discrete energy quanta, are basically of the same type of a nature. However; one of such sets of discrete energy quanta, is here to be conveyed by an isotropically stable Legendre (co)homology, whereas, the other of such sets of discrete energy quanta, is here to be conveyed by an isotropically unstable Legendre (co)homology. That conveyance of a mass-bearing set of discrete energy, that is here to be conveyed by an isotropically stable (co)homology, will consequently tend to bear a greater susceptibility towards a tense of magnetism, than the other of such mass-bearing sets of discrete energy. (This is to where, that mass-bearing cohesive set of discrete energy quanta, that is here to have been conveyed by an isotropically unstable (co)homology, is less likely to bear as strong of an affinity, towards any holonomic substrate of magnetism). SAM ROACH.

Synchronous Superstrings

 When all of those superstrings of discrete energy permittivity, that are here to work to comprise a given arbitrary respective mass-bearing cohesive set of discrete energy quanta, — are to work to bear a synchronous tense of motion, as this is here to be considered, over an evenly-gauged Hamiltonian eigen-metric — this general type of a physical Ward-related condition, will thereby result, in working to cause the directly corresponding herein stated set of discrete energy quanta, to tend to consequently result, in having a tense of isotropic stability. Isotropically stable cohesive sets of discrete energy quanta, tend to have more of a probability of working to bear a tense of group action, — than other cohesive sets of discrete energy quanta, that are, instead, to bear a tense of isotropic instability. To Be Continued! Sincerely, SAMUEL DAVID ROACH.

Group Action And Magnetism

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

Legendre Conveyance Of Mass-Bearing Discrete Energy

 The more that the Legendre conveyance of a mass-bearing cohesive set of discrete energy quanta, is here to be of a De Rham cohomology-related nature, — the quicker that the stated mass-bearing set of discrete energy quanta, will tend to be transversally transferred through space. Sincerely, SAM ROACH. (1989).

Kahler-Based Quotients And Metric-Gauge-Related Pulsation

 The greater the Kahler-Based Quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, — the greater the resultant Majorana-Weyl-Mode is to tend to be. The greater that the Majorana-Weyl-Invariant-Mode is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta , — the deeper that the resultant metric-gauge-related pulsation is consequently to tend to be. Therefore; the greater the Kahler-based Quotient is to be, for a given arbitrary mass-bearing cohesive set of discrete energy quanta, the deeper that the resultant metric-gauge-related pulsation is consequently to tend to be. I will continue with the suspense later! To Be Continued! Sincerely, SAM ROACH. (1989).

Kahler-Based Quotients And Moment Of Inertia

 The higher that the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta, -- the greater that its fractal of Moment of Inertia, will consequently tend to be. Furthermore; the lower that the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta, -- the less that its fractal of Moment of Inertia, will consequently tend to be. Therefore; the greater that the fractal of Moment of Inertia is to be, for a mass-bearing cohesive set of discrete energy quanta, the less often that it will tend to act as being Gliosis to the Kahler-Metric. Furthermore; the less that the fractal of Moment of Inertia is to be, for a mass-bearing cohesive set of discrete energy quanta, the more often that it will tend to act as being Glisos to the Kahler-Metric. To Be Continued! Sincerely, SAM ROACH.

Less Or More Often Gliosis To The Kahler-Metric

The greater that the scalar amplitude of the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta -- the less often that such a mentioned set of discrete energy quanta, is to tend to need to be Gliosis to the Kahelr-Metric. Thereby; the less that the  scalar amplitude of the Kahler-based quotient is to be, for a mass-bearing cohesive set of discrete energy quanta -- the more often that such a mentioned set of discrete energy quanta, is to tend to need to be Gliosis to the Kahler-Metric. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (PHS 1989).

Torsion-Related Tensors

 The more torsion-related tensors, that are here to be directly associated, with the spatial transference of a mass-bearing cohesive set of discrete energy quanta, over a correlative Fourier Transform, the greater that its Kahler-based quotient will consequently tend to be. This will consequently tend to result, in a decrease in the inhibition of the directly corresponding motion, of the said mass-bearing cohesive set of discrete energy quanta. I will continue with the suspense later! To Be  Continued! Sincerely, Samuel David Roach.

Kahler-Based Quotient, And Superstring-Related Fractal Of Momentum

 The greater that the Kahler-based quotient is to be, for a mass-bearing superstring-related phenomenon, that is here to be traveling through a space-related vacuum, -- the more of a superstring-related fractal of momentum, that such a said mass-bearing phenomenology is to consequently tend to exhibit -- in the process by which it is here to be transferred, though the earlier mentioned space-related vacuum. SAM ROACH.(1989).

Torsion Upon Space-Related Vacuum And Dimensionality

 Let us initially consider two different space-related vacuums, of the same three-dimensional volume. Both are to have the same amount of torsion applied to them. One of such space-related vacuums, is to work to bear a higher number of innate spatial dimensions than the other one. That space-related vacuum of the two, of which is here to work to bear a higher number of innate spatial dimensions, will consequently tend to result in working to bear a greater viscosity -- than the other of the two stated space-related vacuums.  Consequently; that space-related vacuum of the two earlier stated ones mentioned, of which is here to work to bear a higher number of innate spatial dimensions, will consequently tend to result in working to bear a greater impedance -- than the other of the two stated space-related vacuums. Samuel David Roach.

Kinematic Torsion Upon Space-Related Vacuum

 The more of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more viscous that such a space-related vacuum will consequently tend to be. A more viscous space-related vacuum, will tend to work to bear a greater physical attribute of impedance. Therefore; the more of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more likely that such a said vacuum, will tend to work to bear a greater physical attribute of impedance. Furthermore; the less of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the less viscous that such a space-related vacuum, will consequently tend to be. A less viscous space-related vacuum, will tend to work to bear a lower tense of a physical attribute of impedance. Therefore; the less of a kinematic torsion, that is here to be exhibited upon a space-related vacuum, -- the more likely that such a said vacuum, will tend to work to bear a lower tense of a physical attribute of impedance. To Be Continued! Sincerely, SAM (1989).

Viscosity Of A Vacuum

 The more viscous that a vacuum in space is to be -- the more impedance that such a said vacuum will tend to exhibit. Consequently; the less viscous that a vacuum in space is to be -- the less impedance that such a said vacuum will tend to exhibit. I will continue with the suspense later! Sincerely, Samuel David Roach.

As To Nature Of i*PI(del) Action

 Any change in either the scalar quantum and/or in the differential geometry, of those partition-based discrepancies, that help to work to comprise the topological manifold of those individually taken correlative superstrings of discrete energy permittivity, that are here to help to work to comprise a cohesive set of discrete energy quanta, will consequently tend to result, in the eminent proximal local presence of the i*PI(del) Action. I will continue with the suspense later1 To Be Continued! Sincerely, SAM ROACH. 

As To Intensity Of Vibrational Delineation

Let us initially consider those given arbitrary superstrings of discrete energy permittivity, that are to work to comprise a directly corresponding given arbitrary mass-bearing cohesive set of discrete energy quanta.  The more intense that the flow of the vibrational delineation of the correlative i*PI(del) Action is to be, for the composite summation of the earlier inferred individually taken respective superstrings, that are here to work to form the said cohesive set of discrete energy quanta, -- the greater that such a kinematic attribute, will tend to reverse-fractal into consequently resulting, in working to form a higher scalar amplitude of magnetism. This is to where, such a general attribute of tendency -- will consequently tend to work to form a greater charge per time (or, in other  words, this stated characteristic of attribution, will consequently tend to work to reverse-fractal, into a superstring-related scenario, to where the eminent external environment of the earlier stated mass-bearing cohesive set of discrete energy quanta, will then tend to work to bear a greater amperage.) To Be Continued! Sincerely, Samuel David Roach. (1989).

As To The Inverse Of A Certain Wavelength

 The flow of the multiplicity of the general process, in which there is here to be an inversion of the kinematic delineation-related tense, of the vibrational wavelength of a thought wave, is a key factor, in the reductional process, in which a given arbitrary thought wave, is thereby to be able to convert into the general topological substrate of ideas. I will continue with the suspense later! To Be Continued!  Sincerely, SAMUEL ROACH.  (1989).

More As To Noether Current, In Relation To Current

 The flow of the vibrational delineation of the i*PI(del) Action, is key at helping to work to form the Noether Current -- and the reverse-fractal of the Noether Current, is the flow of charge (current). SAM.

Flow Of Ebbing -- Discrete Energy

 The flow of the ebbing between discrete energy-related impedance and discrete energy-related permittivity, is key at working to form the general tense of Ward-Cauchy-related pulsation; (pulsation, as taken at the superstring-related level). When the substrate of inverted distance (as in the form of the substrate of physical ideas), is to interact in a Gliossis-related manner, with such an ebbing between discrete energy-related impedance and discrete energy-related permittivity, this helps at working to propagate the general flow of discrete time. To Be Continued! Sincerely, Samuel David Roach.

Harmonic/Anharmonic Magnetic Pulse

 The net resultant harmonic vibrational delineation of the i*PI(del) Action -- of which is here to be of a given arbitrary composite mass-bearing cohesive set of discrete energy quanta -- will consequently tend to reverse-fractal into a harmonic magnetic pulse; Thereby, -- the net resultant anharmonic vibrational delineation of the i*PI(del) Action -- of which is here to be of a given arbitrary composite mass-bearing cohesive set of discrete energy quanta -- will consequently tend to reverse-fractal into an anharmonic magnetic pulse. To Be Continued! I will continue with the suspense later! Sincerely, Samuel David Roach.

As To Vibrational Delineation

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

As To Tensors Of An Eigen Metric Of The i*PI(del) Action

 Let us initially consider a mass-bearing cohesive set of discrete energy quanta. Next; let us consider those individually taken superstrings of discrete energy permittivity, that are here to work to comprise, such a said mass-bearing cohesive set of discrete energy quanta. Let us next work to consider, that we are here to ensue -- in so as to be dealing with a discrete Eigen Metric of the i*PI(del) Action. As such a stated cohesive set of discrete energy quanta, is here to be considered to be translated through a Fourier Transformation -- as this is here to be taken over a directly corresponding Lagrangian, -- the more tensors that are thence to be directly corresponding, to the space-time translation of that composite i*PI(del) Action -- of which is here to be eminent in relation to the maintenance of the conservation of homotopic residue, the more that such a said cohesive set of discrete energy quanta, will consequently tend to reverse-fractal into working to exhibit a heightened tense of magnetism, over the just inferred discrete quantum of time. Sincerely, Samuel David Roach.

Tensors, As To Chern-Simons Invariants

 The more that a cohesive set of discrete energy quanta, is to reverse-fractal-out into working to display a relatively high tense of magnetism, the more (perturbative) Chern-Simons Invariant-related tensors -- that it will consequently tend to work to display -- over a correlative directly corresponding period of time. 

P.S:  Whenever a cohesive set of discrete energy quanta, is to alter in its relative motion in relation to electromagnetic energy -- it (the said cohesive set fo discrete energy quanta) will consequently tend to alter, in its correlative tense of Chern-Simons Invariants. Continued Later!Sincerely, Samuel David Roach.

As To The Torsion Applied To The Light-Cone-Gauge

 The more torsion that is to be applied to an eigenstate of the light-cone-gauge, -- the more likely that this factor, in and of itself, will influence such an inferred wave-related quantum of discrete energy impedance, to tend to consequently result in working to form anharmonic Schwinger-Indices, as these are here to thereby be formed, at the general proximal local region, at which such an earlier mentioned light-cone-gauge eigenstate, is here to be "plucked" like a harp, by its directly corresponding set of gauge-bosons. Sincerely, SAM ROACH.(1989).

Resonant Vibration Of Thought Waves

 Let us consider two different given arbitrary propagated thought waves. Both are here to work to bear the same wavelength, as well as bearing the same intrinsic frequency. Next; let's say that, basically the only difference between the propagational nature of these two different said thought waves, of this particular case scenario, -- is that one of such said thought waves, is to be more harmonically propagated than the other of these two said respective given arbitrary thought waves. That thought wave of the two, -- that is here to be propagated more harmonically, than the other respective thought wave, will consequently tend to result in working to bear a higher resonant vibration, than the other of such said thought waves. SAM.

More As To The Importance Of The Light-Cone-Gauge

 The continuity of Casimer Invariance, is primarily due to the general tendency, of the ever pervasive presence of homotopy. The continuity of homotopy, is primarily due to the general tendency, of the ever pervasive presence of the conservation of homotopic residue. The continuity of the conservation of homotopic residue, is primarily due to the general tendency, of the basically ever pervasive perturbative presence of the Polyakov Action. (Alterations in the Polyakov Action, work to help to allow, for orbifold eigensets that are comprised, eminently by Yau-Exact superstrings, that are to alter in their motion in relationship to light, to be able to better accommodate for the needed flow of the i*PI(Del) Action, in so as to work to help to allow for the general processes of relativity). The Polyakov Action, is primarily due to the general tendency, of the ever pervasive presence of the innate reaction of the light-cone-gauge, towards any correlative changes in the delineation-related allocation of discrete energy quanta --  in their directly corresponding relationship to the motion-related presence of electromagnetic energy. Homotopy -- is the general tendency of discrete energy quanta, to work to bear a web-like field, that is here to work to inter-relate all un-frayed superstring-related phenomenology, via the multiplicity of the interdependent inter-connections, of what I perceive of as being the general tendency, of the ever pervasive presence of mini-string-related segmentation. Sincerely, Samuel David Roach.

Oscillations Of Mini-String--Related Segmentation

 The more spatial dimensions that the immediately external reference-frame of a cohesive set of superstring-related field eigenstates, that are Poincare to the outer Neumman bounds of the topological manifold, that is of such an inferred cohesive set of kinematic mini-string-related segmentation -- that is here to behave as a set, of what I term of here as being physical norm-state-projections (such as zero-norm-state-projections, Campbell norm-state-projections, Campbell-Hausendorf norm-state-projections, and/or Hausendorf norm-state-proejctions) that are thence to be oscillating through, as such an inferred general genus of a cohesive set of segmentation, is here to bear a covariant Gliosis interaction upon a grouping of superstring-related phenomenology, over the durational span of a sequential series of group-related instantons; -- thereby, the more likely that such a said grouping of phenomenology, that is here to bear the kinematic process, of such an inferred interaction of direct contact, is consequently to result in tending to increase in the relativistic perturbation, in the delineation of its inferred facet of correlative covariant spatial translation, over a set period of time, once that such an inferred grouping of superstring-related topological stratum,  is to ensue, in so as to be directly enacted upon. To Be Continued! Sincerely, SAM. (1989).

Perturbative External On-Shell Cohomology-Related Eigenstates

 The general phenomenology -- in which there is here to tend to be the harmonic perturbation in the allocative delineation, of the external on-shell cohomology-related eigenstates, of a mass-bearing cohesive set of discrete energy quanta, as this is here to be taken at a reference-frame, that is external to the covariant spatial translation of such a herein mentioned mass-bearing cohesive set of discrete energy quanta -- helps to work to form the typified entity, of what we tend to think of as being Charge. The general process in which charge is transmitted from one spot to another, over a span of time -- helps to work to form, what we think of as being the phenomenology of Current. I will continue with the suspense! To Be Continued!Sincerely, Samuel David Roach.

Yang And Melting

 The general processes, of which are here to be directly associated with a key attribute of those reductional characteristics, that may be thought of here, as being of the nature of the general type of activity of "yang," may often work to help to facilitate the general activity, of a solid to be able to be more capable of melting into a liquid. This is on account of the two following general conditions:  It takes both the processes of heat And entropy, -- to be able to work to allow for a solid to melt into a liquid. And; the general processes, that are here to be most associated with the application of the nature of "yang" upon phenomenology, -- tends to work to help, in the facilitation of the enablement of entropy. SAM ROACH.