Covariant Isotropically Stable Kahler Manifolds

 When two different proximally adjutant covariant isotropically stable Kahler Manifolds, are here to work to bear an interdependent tense, of a dual gauged spin-orbital momentum, when in co-relation to one another, it will often follow, that both of these two different inferred individually taken Kahler Manifolds, will often tend to consequently work to spontaneously express an asymmetric radial flow, of which is here to bear an anti holomorphic tense of spin, when this is here to be taken, at the Poincare level to the Ward-Cauchy-Related field, that is here to be co-determinable in its covariant proximal local presence, as taken at the vantage-point of its mappable general locus, at the immediately externalized region, which is of such an insinuated co-differentiable Ward-Cauchy-Related field. SAMUEL DAVID ROACH. (PHS1989).

A Kahler Hamiltonian Operator, that works to exhibit a relatively strong covariant tense, of a recursively propagated Poincare delineation, may often tend to exhibit, a relatively enhanced tense, of an inertial-based flow.

A superstring of discrete energy permittivity, that works to express a unitary Lagrangian, may often tend to work to exhibit, a monomial tense of point-fill.  A superstring of discrete energy permittivity, that works to express a binary Lagrangian, may often tend to work to exhibit, a binomial tense of point-fill. Furthermore; A superstring of discrete energy permittivity, that works to express a tertiary Lagrangian, may often tend to work to exhibit, a trinomial tense of point-fill.  

A kinematically propagated Kahler Hamiltonian Operator, that works to bear, both a relatively strong momentum- related Fourier- Related-Progression, &, a relatively strong  inertia-related Fourier- Related-Progression, will often tend to spontaneously work to exhibit, a relatively enhanced general physical characteristic, of expressing an eminently associated “deep” tense, of acting as a compact hermitian topological manifold.  

A recursively spinning, isotropically stable, steady-state, Kahler Hamiltonian Operator, may often tend, to emit a steady charge.

When the Lagrangian-Based motion, of a kinetically transferred Kahler Hamiltonian Operator, is to work to bear, a relatively strong physical attribute, of exhibiting a succinct Fourier-Related-Progression, this may often tend to be eminently associated, with the spontaneous proximal local physical characteristic, of the demonstrative expression, of a strong Heuristic-Based pulse. Furthermore; When the Lagrangian-Based motion, of a kinetically transferred Kahler Hamiltonian Operator, is to work to bear, a relatively strong physical attribute, of exhibiting a resolute Fourier-Related-Progression, this may often tend to be eminently associated, with the spontaneous proximal local physical characteristic,  of the demonstrative expression, of a strong Metric-Based pulse. 

A harmonically oscillating Calabi-Yau Manifold, may often tend to spontaneously emit a hermitian charge.

A sporadically accelerating Kahler Hamiltonian Operator, will generally tend to not be gauge-invariant.  

The more refined, that the eminently associated, Yau-Exact behavior, is to be exhibited as, when in terms of the kinematic activity, of an eminently associated, given arbitrary Kahler Hamiltonian Operator, the more succinct, that the directly related, Fourier-Related-Progression, may often tend to be expressed as, when over the course of time.  

The more isotropically gauged, that the Kahler-Metric is to be exhibited of as expressing, when taken over the course of time, the more resolute, that the proximal local gauge-invariant physical condition, may often tend to be thereupon demonstrated as being, when in terms of the behavior, of the eminently associated, Fourier-Related-Progression, that is here to be of such a case scenario.  

The stronger that the fractal modulus is to spontaneously be, that is of a given arbitrary (Kahler-Based) conductor,  the more amperage, that it may often tend to be able to sufficiently handle, without any viable damage being done, to its eminently related structural integrity. Whereas; The stronger that the elastic modulus is to spontaneously be, that is of a given arbitrary (Kahler-Based) conductor, the more voltage, that it may often tend to be able to sufficiently handle, without any viable damage being done, to its eminently related structural integrity. An eminently associated material, that meets these implicit requirements, when under the physical auspices, of recursive anti gravitational conditions, is potentially ideal, for being able to travel tangentially into outer space, at great speeds, as well as being potentially ideal, for being crucially associated, with the facilitation, of working to form an artificial worm-hole, without any needed Stargate. 

A strong incursion of anti gravity, as imparted upon the eminent field, of a corroborative Kahler Hamiltonian (Operator), may often spontaneously tend to consequently result, in a spontaneously respective heightened Slater-Based Incursion, as imparted upon the topological manifold, of the eminent field, that is here to be directly associated, with the covariant spatial differentiation, of the mentioned corroborative physically transferred, kinematically propagated, Kahler Hamiltonian (Operator).  

Generally Speaking: Lucent thought, may often tend to work to involve, an eminent interaction, between thought waves and imagination waves. Whereas; Cognitive thought, may often tend to work to involve, an eminent interaction, between thought waves and free-will waves.

When The Gravitational Force Stops Its Perturbation -- Riemann Scattering

 When the gravitational force, that is here to be incurred, upon a specific set locus in space and time, is to spontaneously stop, in its initial general occurrence of perturbation, this may, at times, be eminently associated, with the proximal local incursion, of a Riemann Scattering, that may be spontaneously occurring, at this inferred proximal local region, in space and time, over the same general duration, in which the earlier stated gravitational force, is here to have ended, in its inferred initially occurring general process of perturbation. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

Scattered Superstrings -- Chern-Simons Singularties

 Scattered superstrings of discrete energy permittivity, tend to work to bear Chern-Simons singularities -- at the locus at which these are scattered. TO BE CONTINUED! SINCERELY, SAMUEL ROACH.(1989).

Perturbation Of Gauged-Action

 When a Noether-Based superstring-related gauged-action is to be perturbative,  it will thereby often tend to spontaneously work to bear a Lagrangian-Based Chern-Simons singularity, at the locus at which the said gauged-action is to become perturbative.UNTIL NEXT TIME; HAVE A GREAT DAY! SAMUEL. 

Alteration In Type Of Expansion -- Lagrangian-Based Chern-Simons Singularities

 When a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, is to spontaneously alter, from exhibiting a euclidean expansion, into ensuing to exhibit a Clifford expansion, the stated cohesive set of discrete energy quanta, at the locus in which such a change in the type of expansion, that is here to be exhibited in its consequentially resultant kinematic display, will often tend to work to bear a certain given arbitrary respective tense, of a Lagrangian-Based Chern-Simons singularity. Likewise; When a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, is to spontaneously alter, from exhibiting a Clifford expansion, into ensuing to exhibit a euclidean expansion, the stated cohesive set of discrete energy quanta, at the locus in which such a change into the type of expansion, that is here to be exhibited in its consequentially resultant kinematic display, will often tend to work to bear a certain given arbitrary respective tense, of a Lagrangian-Based Chern-Simons singularity. TO BE CONTINUED! SAM.

More, As To Pulse Of Schwinger-Indices

 The quicker and/or deeper the wave-tug that is here to be incurred upon a set of one or more second-order light-cone-gauge eigenstates, by their directly corresponding respective gauge-bosons, -- the stronger that the consequentially formed pulsation of Schwinger-Indices that will often tend to result in being formed, as such said Schwinger-Indices are thence to result in being propagated out tangentially, From their initial locus of formation. I WILL CONTINIUE WITH THE SUSPENSE LATER! SINCERELY, SAM ROACH.

My Current Conceptualization, As To The Potential Existence Of "Nothingness"

 To my present conceptualization, I do NOT believe in the actual existence of "nothingness," in and of itself. To my current perception, I believe, -- that the topological stratum that the Logos was to be traveling through, as it (the Logos) was heading towards the region-related locus of the core of the "Big-Bang," at which it was to commence for its interaction with the implied "topological manifold," of such a stated "core" of phenomenology, in so as to work to form the ensuing created multiverse, (Note; I call what worked to cause the "Big-Bang," the Logos, to where I personally believe in intelligent design.), was here to be a general type of an immense surrounding "topological manifold" of sorts, of which could be potentially described of, as being an extraordinary permeable region, of "inverse-impedance." Sincerely, SAM ROACH.

Another Refinement — As To Anti Holomorphic Kahler conditions

 Here is another refinement that I have just thought of lately, as to more properly perceiving my particular model of string theory that I have been working to develop:

Let us initially imagine a given arbitrary Noether-Based mass-bearing cohesive set of discrete energy quanta, that is here to be starting out — moving in a hermitian-related manner, along its directly corresponding Lagrangian-Based path. Let us next stipulate, that such a said cohesive set of discrete energy, is here to be in the process of being propagated in a certain manner, to where it is here to be spatially transferred, over a proscribed given arbitrary span of time, as a maintained six-spatial dimensional physical entity. Next; let us say, that this herein inferred set of energy quanta, is to all of a sudden, spontaneously alter from its initial tense of a hermitian-related flow, — to where, at a certain given arbitrary locus in space and time, as this is here to be taken along the mappable-tracing of its directly associated Lagrangian-Based path, such a said set of energy quanta is to spuriously change in seven spatial derivatives,  to where again, this is here to be happening at the earlier implied given arbitrary locus in space and time, at which the inferred sudden and spontaneous alteration of projected trajectory, is here to be occurring. This just inferred perturbation of sorts, is therefore to work to signify, that the perturbative locus at which such an alteration is here to occur, is then to act or operate, as a first-order Lagrangian-Based Chern-Simons singularity. Let us next say, that this said “singularity,” is to be happening in a “cross-product-related manner” (via the ‘vantage-point” of the holomorphic positioning of its angular momentum eigenstate)  — to where, —although this will tend to work to alter what the holomorphic direction of the cohesive set of energy is to specifically be projected in, that this will, however, tend to not work to form any viable set of anti holomorphic Kahler conditions. Yet; if instead, the inferred sudden and spontaneous alteration of projected trajectory, is here to be occurring as Similar to before, Yet, to where the directly associated first-order Lagrangian-Based Chern-Simons singularity that is here to be formed, is to be happening, instead, in a “dot-product-related manner” (via the “vantage-point” of the holomorphic positioning of its angular momentum eigenstate) — that this  particular tense of a genus of a Lagrangian-Based Chern-Simons singularity, will thereby result in tending to work to form a set of anti holomorphic Kahler conditions, — as the earlier mentioned mass-bearing cohesive set of discrete energy quanta, is thence to be pulled into a potentially different genus of an alteration in its general genus of holomorphic topological sway, as this is here to be taken along its correlatively morphed Lagrangian-Based Flow. This second general genus of a perturbative Lagrangian-Based Flow, is thereby to tend to be more likely to work to form a set of physical conditions, by which the herein described cohesive set of discrete energy quanta, may have a greater potential than in the other case scenario, to become Gliosis to the Kahler-Metric. To Be Continued! Sincerely, SAM ROACH. (1989).

More As To Locus Of Cotangent Bundle

 The general multiplicity of a locus, at which the cotangent bundle is here to be converged upon, -- works to appertain to the directly corresponding genus of a locus, at which such an inferred Laplacian-Based setting, is here to display the distributed delineation -- of a cohesive set of discrete energy quanta. SAM.

Dimensional-Related Pulsation, And The i*PI(Del) Action

 Whenever a given arbitrary Noether-based mass-bearing cohesive set of discrete energy quanta, is to alter in its dimensional-related pulsation, -- not only will it consequently tend to work to bear a metric-related Chern-Simons singularity, at the proximal locus, at which such a said alteration in dimensional-related pulsation is to occur, yet, such an inferred set of discrete energy, as such a change is here to be occurring, will simultaneously (at the proximal locus of a central coni-point), tend to be undergoing an alteration, in either its speed and/or in its directional delineation, in relation to light, in the process of doing so. It follows then; that whenever  there is to be a gauged-action, by which there is to be the proximal local occurrence, at which there is to be the eminent presence of a metric-based Chern-Simons singularity, this general type of a common occurrence, will tend to be directly associated, with the eminent presence of what I term of, as being a general physical phenomenology, that I call here, the i*PI(Del) Action. Sincerely, SAM ROACH. (1989).

More As To Cohomological Eigenstates, Eigenindices

Cohomological eigenstates may either be abelian or non abelian groupings, that latch at a locus that is proximal local to the topology of discrete energy; whereas -- cohomological eigenindices are discrete motions of such abelian or non abelian groupings, that work to indicate the presence of the thence proximal local said cohomological eigenstates.  Sincerely, Samuel David Roach.

Oscillation Of Wave-Based Discrete Energy Impedance

Individually taken light-cone-gauge-eigenstates -- are wave-based discrete increments of energy impedance.  The vibrational oscillations of light-cone-gauge eigenstates, are propagated along the Rarita Structure, in order to work to form those Schwinger-Indices -- that not only come together in so as to work to form the phenomenology of gravitational waves, yet, such thus formed Schwinger-Indices are also produced, in order to operate in so as to work to effect the condition of which general genus of force is to be implemented at what locus, over the course of that incurred multiplicit eigenmetric -- in which such forces in the substringular are to both be produced and functional over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Rate Of Acceleration And Homotopic Residue

As a given arbitrary superstring of discrete energy permittivity is to increase in either its acceleration or in its deceleration over time, in terms of working to bear a respective increase or a respective decrease in the rate, that the directly corresponding Lagrangian-based superstring is to be transferred either respectively faster or slower from one point to another over time -- it is then to increase in the rate by which such a said superstring of discrete energy permittivty is to either respectively lose partition-based discrepancies (if it is increasing in its said acceleration) or to gain partition-based discrepancies (if it is increasing in its said deceleration), over an evenly-gauged Hamiltonian eigenmetric.  This will then mean, that such a said superstring -- will then be in such a condition -- to where it will then be increasing in the rate of its exchange of such partition-based discrepancies.  This will then mean, that an increase in the acceleration of a superstring of discrete energy permittivitiy, or, as well, an increase in the deceleration of such a said string -- will then result in an increase in the rate of the perturbation of the delineation of that homotopic residue, that is proximal to the codifferentiable-related variable locus, in which such a so-mentioned superstring is to be transferring through -- in such a manner to where this is to happen, via the kinematic motion of its directly associated Lagrangian over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Relatively Dense Centralized Knotting

The strong force is multiplict at a locus, at which there is an eigenstate of the centralized knotting of the Rarita Structure.  Gravitational waves tend to move outward and perpendicular to the transversal medium that these are here to be moving through, over time.  The strong force is that force that works to inter-bind those subatomic particles together, in so as to work to bring phenomenology together -- such as that force that works to bring quarks and/or leptons together in so as to form protons, neutrons, and electrons.  A high density of subatomic particles will tend to mean that there will thereby be a high density of atoms.  A relatively high density of atoms eludes to the condition of a relatively high tense of gravity.  The more dense that the delineation of eigenstates of the centralized knotting of the Rarita Structure is, the more that the gravitational force will tend to act upon its surroundings -- in so as to work to push-in such external phenomenology upon itself.  Therefore -- the more dense that the delineation of the strong force is, the more that the gravitational force will tend to act upon its surroundings -- in so as to work to push-in such external phenomenology upon itself.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gravity Waves And Holomorphicity Of Impact

When one is to be considering the general angle, by which any one given arbitrary respective photon is to strike the externalized core-field-density of the correlative light-cone-gauge eigenstate -- that it is to come into contact with, in a Gliosis-based manner -- to where if the directly corresponding superstring and its directly corresponding counter string are then to be positioned at the relative left to the extrapolated positioning that one were to have, if one is to take the vantage-point of the norm-to-holomorphic positioning of the said photon -- in the direction in which the eminent scattering is to be made upon that general proximal locus, -- then, the consequently formed Schwinger-Indices that are thence to be made will then tend to have a higher expectation value in so as to be of a harmonic vibration.  Yet, if one is to be considering the general angle, by which any one given arbitrary respective photon is to strike the externalized core-field-density of the correlative light-cone-gauge eigenstate -- that it is to come into contact with, in a Gliosis-based manner -- to where if the directly corresponding superstring and its directly corresponding counter string are then to be positioned at the relative right to the extrapolated positioning that one were to have, if one is to take the vantage-point of the norm-to-holomorphic positioning of the said photon -- in the direction in which the eminent scattering is to be made upon that general locus, -- then, the consequently formed Schwinger-Indices that are thence to be made will then tend to have a higher expectation value of being of an annharmonic vibration.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Terms Cohomologies Versus Ghost Anomalies

That description of the physical memories, as to the where, the when, and the how, that the multiplicit substringular eigenstates have differentiated over time -- as may be described by the term that I call ghost anomalies, -- works to imply the temporal nature of the existence of the so-eluded-to  individually taken cohomological entities.  This is since the presence of an anomaly -- works to imply the existence of something that may rarely be both significantly detected and apprehended as both real and observable, at any specific given arbitrary locus.  Whereas -- the eigenstate of a given arbitrary respective cohomology, may simply refer to the existence of the physical memories as to the where, the when, and the how, that the multiplicit substringular eigenstates have differentiated in the arena of space-time-fabric in general.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Lagrangian-Based Cohomological Generation

Let us initially consider one given arbitrary orbifold eigenset -- that is in a state of superconformal invariance, -- at one respective given arbitrary proximal locus.  Such a respective orbifold eigenset, is here to be of a Rham-based cohomology -- that is here to tend to generate as much cohomological eigenindices as it is here to degenerate, over a gauged-metric, that is of an even Hamiltonian metrical function.  Such an orbifold eigenset is here to tend to be of a Yau-Exact nature, in so long as the topological stratum that works to comprise the said orbifold eigenset, is of a Calabi-Yau nature.  In this case, both the resultant formed Lagrangian-based singularities and the resultant formed metrical-based singularities, will tend to be of a hemitian nature, over the so-eluded-to proscribed guaged-metric.  Let us next say, that a group-attractor is to act upon the holonomic substrate of the said orbifold eigenset -- to where the so-stated eigenset is to then to all of the sudden act, in so as to then be generating a net of cohomological eigenindices, in the relative forward-holomorphic direction.  Now, the orbifold eigenset in question, is now to be of a Doubolt-based cohomological setting, instead of being of a Rham-based cohomological setting, -- as the said orbifold eigenset is now to no longer be of a superconformally invariant nature.  The orbifold eigenset is to then to work to bear at least one set of Lagrangian-based Chern-Simons singularities, -- to where it is to consequently to bear at least one respective set of complex roots, that may here work to describe the Ward-Cauchy-based nature of such path-related resultant changes, that are in the differential curvature that is here to be related to the perturbated motion of the said orbifold eigenset.  In so long as the so-eluded-to set of superstrings that work to comprise the one respective Hamiltonian operator of this case (the said orbifold eigenset that is here being discussed), are not be alter in the nature of their group-related pulsation -- over the duration of the so-eluded-to changed nature of the motion of the said orbifold eigenset -- then, there isn't the tendency of the formation of metrical-based Chern-Simons singularities in the overall said process.  I will continue with the suspense later!  To Be Continued!
Sincerely, Sam Roach.