Metric Singularity And Torsion Of Pulse

Let us consider an orbifold eigenset -- that is here to be moving through space and time, over a smooth  monomial-related tense of a Lagrangian-based path; in which such a said eigenset, is consequently to be associated with the same number of directly corresponding directorals, in conjunction to the Fourier-related translation of the said orbifold eigenset, along its said Lagrangian-based path.  Let us next say that such an inferred eigenset, is here to either bear an increased torsion upon its correlative proximal local pulse, Or, a decreased torsion upon its correlative proximal local pulse.  In the process, what is to amount to here, as being either a respective increase in torsion or a respective decrease in torsion -- upon the pulse of the here stated orbifold eigenset, --  will almost certainly tend to result, in a consequential metric-related set of Chern-Simons singularities -- as this is here to be physically applied to the holonomic substrate of the topological stratum of the said orbifold eigenset, -- at the proximal region, at which such a change in the inferred tensor-related scalar amplitude of torsion, is here to enact such an inferred perturbation, upon the here stated orbifold eigenset, -- over an evenly-gauged Hamiltonian eigenmetric. Sincerely, Samuel David Roach.

Chern-Simons Invariants

Let us initially consider two different orbifold eigensets, that are here to be moving in a covariant manner -- over an evenly-gauged Hamiltonian eigenmetric.  Both orbifold eigensets are here to be moving at both the same transversal rate, And, at the same radial rate, -- in their relation to light.  Furthermore; both orbifold eigensets are also here to work to bear both the same angular momentum And the same spin-orbital momentum, -- over the same earlier inferred evenly-gauged Hamiltonian eigenmetric.  Otherwise, both of these said orbifold eigensets are to be basically of the same nature and behavior; except that one of these said eigensets is to work to bear a higher number of directly associated spatial dimensions, that are here to be proximal local to the topological stratum of the said orbifold eigenset, -- than the number of spatial dimensions that are here to be directly associated with the proximal local topological stratum of the other stated orbifold eigenset.  In this particular case; that orbifold eigenset, that is here to work to bear a greater number of spatial dimensions, -- will consequently tend to work to bear a greater flow, in the rate of the perturbation of its directly corresponding Chern-Simons Invariants -- when this is here to be taken, over that process, in which such an earlier implied covariant tense of a Hamiltonian eigenmetric is here to occur. Sincerely, Samuel David Roach.

Scalar Amplitude Of Gravitational Force And Rate Of A Certain Tense Of Substringular Recycling

The greater that the  scalar amplitude is to be, of the gravitational force that is here to applied upon a certain stratum of a mass-bearing region of phenomenology, -- the higher that the rate will consequently Tend to be, of the Ward-Cauchy-related indistinguishably different recycling of the directly corresponding Neilson-Kolosh cohomology-related eigenstates, that are here to be proximal local to the earlier inferred respective stratum of mass-bearing region of phenomenology. Sincerely, Samuel David Roach.

Wave-Tug, Noether Flow, And Approaching Light Speed

Let us consider a mass-bearing orbifold eigenset, that is here to be initially traveling transversally in its innate holomorphic direction, in relation to the motion of light.  The more that the Legendre homology-related grouping, that is here to be tugging-along the earlier mentioned mass-bearing orbifold eigenset, in its said implied innate holomorphic direction, -- to where this is here to be working to move the implied respective eigenset, in a linear-based transversal direction (in so far as the curvature of space-time-fabric is to make this feasible enough), in the directorial-related path, that is here to be of the initially inferred forward-holomorphic direction; that is here to be innate to the particular genus of Ward-Cauchy-related field, that is of the given arbitrary orbifold eigenset of this respective case scenario -- over the course of a tense of Noether Flow, the closer that such a said mass-bearing orbifold eigenset will consequently Tend to approach the speed of light. Sincerely, Samuel Roach.(PHS, Class of 1989).

Rate Of Flow In the Perturbation Of Chern-Simons Invariants

Let us initially consider two different given arbitrary orbifold eigensets, that are both to work to bear the same scalar amount of cohomology-related generation (to where, this will tend to reverse-fractal into both orbifold eigensets, working to be associated with the same scalar amount of charge.)  Both of these just mentioned orbifold eigensets, are here to be  basically of the same nature and behavior, except that one of these said orbifold eigensets is to work to bear a greater scalar amplitude, in the rate of the flow of the perturbation of its directly corresponding innate Chern-Simons Invariants, than the other said orbifold eigenset.  Based upon the directly previous stipulation, that orbifold of this particular case -- that is here to work to bear a greater scalar amplitude, in the rate of the flow of the perturbation of its directly corresponding innate Chern-Simons Invariants, will Tend to bear a higher scalar amplitude in the conglomerate rate of its directly associated i*PI(Del) Action, than the other of the two here mentioned orbifold eigensets, that was stated here, in this particular case.
I will continue with suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The General Idea Of What Created Time

Since the Main Influence that the thought force works to form, as Acting upon the Main Influence that the force of gravity works to form, works to help at forming time, -- which is, in general, to be operating upon a directorial-related metric times a constant, that is here to be operating upon a tense-related series of relative motion (as this is all to be divided by "8*PI^2"), this then works to Imply, that time was originally created by the Interaction that was here to exist, between the Logos (the intelligent design), And the inertial tense of that fabric; that was here to initially be latent at the core of the "Big-Bang."
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Re-Iterative Alteration Of Charge

Let's initially consider a charged mass-bearing orbifold eigenset, that is here to be traveling via a path, that is iterative in its tense of Lagrangian-related flow.  The Ward-Cauchy conditions of its said iterative tense of Lagrangian-related flow is consistent, except that the propagation of the said orbifold eigenset is to go from working to bear the constraints of a unitary Lagrangian, to then working to bear the constraints of a binary Lagrangian, to then going back into working to bear the constraints of a unitary Lagrangian, and so on, -- as the propagation-related projection of the said eigenset of such a case, is to be reiterating in its tense of a flow of motion -- over a directly corresponding repetitive evenly-gauged Hamiltonian eigenmetric.  Consequently; the said orbifold eigenset of such a particular case, will then tend to go from bearing a certain scalar magnitude of cohomology-related generation, to working to bear a higher scalar magnitude of cohomology-related generation, into ensuing to bear its initial inferred scalar magnitude of cohomology-related generation, and so on, -- as the here implied set of discrete quanta of energy, that are here to operate in so as to perform one specific function, is to propagate in a repetitive tense of a path-related flow of motion, -- that is otherwise of the same general genus of substringular boundary conditions.  Such a re-iterative alteration of charge, will then tend to work to reverse-fractal into working to form a Ward-Cauchy-related tense of an initial scalar magnitude of charge, into consequently altering into working to form the reverse-fractal of a higher scalar magnitude of a Ward-Cauchy-related tense of charge, while then going back into working to form the reverse-fractal of the initially inferred scalar magnitude of a Ward-Cauchy-related tense of charge, and so on.  Such a process of a re-iterative alteration, or perturbation of charge, will tend to occur, in so long as the motion of the said orbifold eigenset, is to be consistent, With the exception of going from working to bear a unitary Lagrangian-based flow, into working to bear a binary Lagrangian-based flow, and back again, -- as the said eigenset is here to be reiterating, in its directly corresponding pattern of a flow of motion, over a discrete quantum of time.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Metric-Related Relative Motion

When one is initially to take the basic forces of nature; while then embedding upon these inferred forces, a correlative generic Chern-Simons-Invariant gauge-action -- this works to indicate the Main Influences of physical nature, as operating upon a respective system of a metric-related tense of relative motion, -- by which one is here to be able to mathematically work to bear the inferred determined Main Influence "out in front" of a metric-related operator, that is here to be operating upon some sort of a system, that is here to involve a tense of relative motion.

For Instance:

Let's say that one were to take a situation, in which there is here to be two different Chern-Simons-Invariant gauge-actions.  One is to be directly relating to the thought force, while the other is to be directly relating to the force of gravity.  Let us next say that both of these inferred gauge-actions, are to be of a cotangent bundle of R3. Let's next say, that both of these said respective gauge-actions -- are here to work to bear the same Pattern of a Lagrangian-related trace.  Next -- chose your Ads equations, while then working to determine what the two individually taken Chern-Simons-Invariant gauge-actions are to be.  At this point, work to determine what the two individually taken Main Influences are to be, as derived from the ante descendant math implied here, after figuring-out what these just determined gauge-actions are. Now, couple these two said gauge-actions -- by taking the product that is here to exist between the two said "actions."  (A.K.A. multiply these together.)  Next; take what one would then work to determine, as being the mathematical expression of the earlier implied product of the two considered Main Influences, With the system of metric-related relative motion, that it is here to be operated upon.  What one would get, is a constant times "seconds" (time) -- operating upon a directorial-related metric, that is here to be operating upon the following generic mathematical substrate:   (a constant times "jerk" (change in acceleration per time) + a constant times acceleration + a constant times velocity + a constant times metric + a constant times pulse) times a constant, while then dividing this whole thing by 8*PI^2.  In this case, then, when working towards determining the product, that is here to exist between two of the main influences of physical nature From two of the basic forces of nature, one is here to consequently get a value of "time" operating upon a metric of relative motion. Sam Roach.

Differences In Types Of Lagrangian And Scalar Amount Of Charge

Let's say that one were to be considering two different charged mass-bearing orbifold eigensets.  Let's say that both of such said orbifold eigensets, are to work to bear the same covariant relativistic transversal velocity, in their relationship to the motion of electromagnetic energy.  Let's next say that both of such said orbifold eigensets, are here to work to bear the same scalar amplitude of both a tense of spin-related momentum  and of a tense of orbit-related momentum, over the evenly-gauged Hamiltonian eigenmetric -- in which the covariant motion of both of such said orbifold eigensets is here to be considered.  One of such said orbifold eigensets is here to be traveling via a binary Lagrangian, whereas the other of such said orbifold eigensets is here to be traveling via a tertiary Lagrangian. The orbifold eigenset that is to be considered in this particular case, that is here to be traveling via a tertiary Lagrangian, will then have more of a tendency of working to bear a greater scalar amount of charge. To Be Continued!  Sincerely, Samuel David Roach.

An Editorial Thought That Came To My Mind

The following post is just an editorial set of thoughts that's been going on in my head, so I figured that I would "run" it by you.  Again, the following is just an editorial:

Here is an analogy between the 7 Main Influences Of physical nature, and their metaphysical corollaries:

1)  Ideas are analogous to Mind.

2)  Metric-Gauge ("Force-Fields") are analogous to Truth.

3)  The i*PI(del) Action is analogous to Spirit.

4)  The Majorana-Weyl-Invariant-Mode is analogous to Soul.

5)  Charge is analogous to Love.

6)  Inertia is analogous to Principle.

And 7)  Entropy is analogous to Life.

Also,  just as the interaction that is here to exist between the seven Main Influences of physical nature, works to help to allow for the physical condition of homotopy;  The interaction that is here to exist between their seven metaphysical corollaries, works to help to allow for the metaphysical Presence of the Logos.

To Be Continued!  Sincerely, Samuel David Roach.

Chern-Simons Invariant-Related Action And The i*PI(del) Action

Let's initially consider two different orbifold eigensets, that are here to work to bear a covariant-related motion in relationship to one another.  Both are here to be similar but different, except for one main factor, -- even though both of these said orbifold eigensets, are here to work to bear the same transversal change in motion, -- when in respect to the motion of electromagnetic energy.  Here is the one main difference between the two so-inferred eigensets; one of these said orbifold eigensets, is to work to bear a greater scalar amplitude of a tense of spin-orbital momentum than the other said orbifold eigenset.  The said eigenset of the two, that is here to work to bear a greater scalar amplitude of a tense of spin-orbital momentum than the other inferred eigenset -- is then to consequently work to tend to bear a greater scalar amplitude of torsion, that is here to be applied to the topological stratum of its directly corresponding entity of holonomic substrate, -- than the amount of a scalar amplitude of torsion that is here to be applied to the other mentioned orbifold eigenset of this particular case.  The here inferred Ward-Cauchy-related Hamiltonian Operator, that is here to tend to work to bear a greater torsional force that is here to be applied to the topological stratum of its directly corresponding entity of its holonomic substrate, -- will then consequently tend to bear a greater plateau of a change in motion, than the other here mentioned inferred Ward-Cauchy-related Hamiltonian Operator.  This will thus work to help in causing there to tend to be more of an applied tense of an i*PI(del) Action, that is here to be "geared" upon this said orbifold eigenset, which is also here to work to bear a greater tense of a torsion of which is here to be applied to its topological stratum, than what is here to be applied to the other said eigenset of the two.  This will thence tend to work to cause the so-inferred orbifold eigneset, that is here to work to bear a greater tense of torsion -- that is here to be applied upon it, to work, as well, to bear a greater scalar amplitude of a Chern-Simons Invariant-Related Gauge-Action, that is here to be applied upon it.  Furthermore; in this particular case, the orbifold eigenset that is here to bear the greater tense of a Chern-Simons-Invariant operation, will then tend to work to be associated with a greater charge, than the other said orbifold eigenset will tend to be associated with, -- over an evenly-gauged Hamiltonian eigenmetric.  To Be Continued!  Sincerely, Samuel David Roach.

How "Tightly-Knit" Your ds For Integration Is

Whether or not one is to consider a Ward-Cauchy-related condition, to be of either a Fourier-related-type situation or of a Laplacian-related-type of a situation, in part, may often be relative to how "tightly-knit" your "ds" of integration is here to be.  For instance, if you are here to be involved with an occurrance, that is here to be happening, in full, over a thousandth of a nanosecond, then, one may then concur to be able to think of charge in and of itself, in lei of being of a Laplacian-related manner of a Ward-Cauchy scenario.  Yet, if one were, instead, to be involved with an occurrance, that is here to be happening, in full, over a significantly smaller duration of time (let's say, for only 10^(-41) of a second), then, one may then concur to be able to think of charge in and of itself, in lei of being of a very tightly-knit Fourier-related manner of a Ward-Cauchy scenario.  This eludes to the general stipulation, -- that whether one is to be considering something (let's say for instance, "charge" in and of itself) to be of a Laplacian-based situation (like a snapshot), or whether one is to be considering something (let's say for instance, "charge" in and of itself) to be of a Fourier-based situation (as something that is here to be happening over a duration), is at least partially dependent upon how tightly-knit your ds of integration (the "slivers" of time, that are here to operate as the here to be considered smallest parts of time, for any one given arbitrary scenario) are to be wavered-out to be.  I will continue with the suspense later!  To Be Continued!  Sincrely, Samuel David Roach.

Some Interesting Stuff About Charge

As an initial ansantz (as to here to be starting with something that people would generally tend to know), current is the basic relationship of charge per time.  Yet, the "equivalence" of charge, as here to be taken at an extremely small quantity of such a general genus of phenomenology, is an analogous relationship of the "i*PI(del) Action" per time.  To Be Continued!  Sincerely, Samuel David Roach.

A Strange Irony

Here is a strange irony, that I am considering in my model of string theory:

Although the Force of pressurized vacuum Divided by the point commutative Force is analogous to substringular impedance, the Main Influence that the force of pressurized vacuum works to form Multiplied by the Main Influence that the point commutative force works to form, is, ironically enough, as well, analogous to substringular impedance. I consequently propose to notion, that I am considering that the Majorana-Weyl-Invariant-Mode is to happen to be analogous to a tense of substringular impedance. Sincerely, Samuel David Roach.

An Interesting Analogy

Even though what I term of as being the force of pressurized vacuum, the point commutative force, and also the electromotive force, -- are three different basic types of force -- here is an analogy that I think is interesting:

The force of pressurized vacuum is to "voltage," what the point commutative force is to "amperage."
I will continue with the suspense later!  To Be Continued!  Sincrely, Samuel David Roach.

Analogy Between The i*PI(del) Action And The Majorana-Weyl-Invariant-Mode

The i*PI(del) Action is to cohomology and thence to charge, in an analogous manner to what the Majorana-Weyl-Invariant-Mode is to mass.I will continue with suspense later!To Be Continued!Sam!

The Units For The i*PI(del) Action

The expression (in units) that is here to be utilized, for the physical representation of the "i*PI(del) Action" -- is in terms of an extremely small number times the units of Coulumbs*Seconds.  Sam Roach.

Spurious Perturbation Of Inertia

When there is to be a spurious perturbation in the flow of the fractal of inertia, that any one given arbitrary orbifold eigenset is to exhibit, such a said orbifold eigenset will then consequently tend to bear a metric-related Chern-Simons singularity -- at the proximal local region at which there is to be such a said spurious perturbation in the flow of the fractal of its inertia. Samuel David Roach. (1989).

Cycles Of Pressurized Vacuum

During group-related instanton, that tense of a pressurized vacuum, -- that is here to exist in-between the countless eigenstates of mini-stringular segmentation -- is to bear a relatively high scalar amplitude of intensity.  Whereas; when one is here to be considering iterations of the generally unnoticed duration of Ultimon Flow, that tense of a pressurized vacuum, -- that is here to exist in-between the countless eigenstates of mini-stringular segmentation -- is to bear a relatively low scalar amplitude of intensity. I will continue with the suspense later!  To Be Continued! Samuel Roach.

Flow Of Phenomenology And Pressurized Vacuum

The higher that the scalar amplitude is, of the intensity of that tense of a pressurized vacuum -- that is to be of the exhibition of space-time-fabric, that is here to exist at the general physical stratum, that is here to be distributed at those proximal local regions, that are to be displayed in-between the countless eigenstates of mini-stringular segmentation, -- then, the more inhibited that the resulting flow of superstringular phenomenology, that will then tend to be transferred through the multiplicit Hamiltonian operand, that these are here to be translated through, in a Fourier-related manner.  Consequently; the lower that the scalar amplitude is, of the intensity of that tense of a pressurized vacuum -- that is to be of the exhibition of space-time-fabric, that is here to exist at the general physical stratum, that is here to be distributed at those proximal local regions, that are to be displayed in-between the countless eigenstates of mini-stringular segmentation, -- then, the less inhibited that the resulting flow of superstringular phenomenology, that will then tend to be transferred through the multiplicit Hamiltonian operand, that these are here to be translated through, in a Fourier-related manner. Samuel David Roach.

Gauge-Actions And Monomial-Based Path

A set of gauge-actions are said to bear a monomial tense of a path, -- when this said set of gauge-actions, are to only work to bear one pattern of a Lagrangian-based path.  Let me explain this here in more detail.  A Lagrangian is the actual motion that energy is to exhibit.  Consequently; when one is here to be dealing with a set of discrete quanta of energy, -- the correlative Lagrangian, is the actual motion that the said respective set of discrete quanta of energy, is here to exhibit.  Next;  Let's say that there are to be four different superstringular activities, that are here to be occurring at a general proximal local region.  Whether or not the scalar amplitude of each of these inferred Ward-Cauchy-based Fourier-related activities are to be of the same magnitude, each of these superstringular activities is here, in this particular case, to exhibit the exact same route of transfer Of their individually taken overall discrete quanta of energy (one overall set of discrete quanta of energy for each individually taken set of gauge-actions).  Since each of the four said sets of gauge-actions, are here to be displaying the same path, by which their correlative energy is to be transferred, -- there is here to be only one type of pattern of Lagrangian-based path to be considered here.  One could then, theoretically, map-out the actual path of each of these sets of gauge-actions upon each other, in a Laplacian-related manner, -- and, these would consequently, then, be able to overlap.  Consequently; there is here to be only one type of overall path of energy, that is here to be exhibited.  This, thereby, works to constitute a monomial tense of a path. To Be Continued! Sincerely, Samuel David Roach.

Hamiltonian Operators And Yukawa Couplings

When two different Hamiltonian Operators act upon one another, in so as to multiply their action -- this is a general given arbitrary example of a Yukawa Coupling. Sincerely, Samuel David Roach.

Fields

The integration of the countless metric-gauge eigenstates that are here to exist in the superstringular -- work to help form the respective vast array of superstringular fields. Sincerely, Sam Roach.

Mass And Metric-Gauge

Mass -- at its most fundamental level -- tends to exist as being Equivalent to a Yukawa Coupling between metric-gauge and charge. Sam Roach.

Ideas And Time

Even though time is actually the multiplicit duration of the sequential series of group-related instantons, time is Equivalent to acting as a Yukawa Coupling between ideas and inertia. Sincerely, Sam Roach.

Some Neat Stuff As To The Majorana-Weyl-Invariant-Mode

The multiplicit Majorana-Weyl-Invariant-Mode is equivalent to a Yukawa Coupling, that is here to exist  between a set of one or more metric-gauge eigenstates And the i*PI(del) action. Sam Roach.

Cox Rings And Cohomology-Related Eigenstate

Those external fringes that are of a given arbitrary cohomology-related eigenstate, that are here to be of a closed-loop superstringular field, that are here to work to bear a common radial-related center of its spatial dimensionality, are here to act as a Cox Ring in the substringular. Sincerely, Samuel Roach.

Cox Rings

Ring-Like orientations of Del Pezzo Spaces, may be thought of as being Cox Rings. Sam Roach.

Del Pezzo Spaces

Mathematically-Derived spaces, that are here to work to bear an orientation -- via the application of a Grobner Basis, -- may be termed of as being  Del Pezzo Spaces. To Be Continued!  Samuel Roach.

Interesting Stuff As To Grobner Bases

Let's consider what is meant to be determined as a Grobner Basis:

Let's say that one is to have a point particle.  It is theoretically to be of zero spatial dimensions.  Consequently; its surrounding spatial dimensionality, is theoretically here to be "infinite" in its number of spatial dimensions.  Next; one may take certain basic differential geometrical-related mathematical stipulations, about the dimensional relationships of certain spaces, that are here to be related to both the existence and the motion of such a theoretical point particle, both as to what may potentially be an element of what, what may be in union to what, what may intersect what, etc., -- based upon the basic mathematical operations of addition, division, multiplication, and subtraction.  Consequently; one may then work to determine an eigenbasis, that is here to work upon a given arbitrary space, in a Laplacian-related manner -- that is here to work to involve a stipulation, that involves the relationship of one point particle To a stipulation that involves the relationship of another point particle, -- to where the relationship that is here to work to involve the two inferred point particles, is then to be of either a Real Riemann Gaussian-related association, or of a Li-based Gaussian-related association.  Such a general tense of an eigenbasis, may then be utilized, to work to determine as to what actual point-like spaces are more likely to be relatively adjacent to other actual point-like spaces, -- given how such point-like spaces are here to be acting, over time. Such a general tense of an eigenbasis, may be thought of as a Grobner Basis.  Sincerely, Samuel David Roach.

More As To Torque And Metric-Gauge

The more torque per metric-gauge that a given arbitrary orbifold eigenset is to be applying, upon the directly corresponding Hamiltonian operand that such a said respective orbifold eigenset is to be moving through, over time, -- the more of a holomorphic-related drive or wave-tug, that will consequently tend to be applied by such a stated eigenset, upon the space-time-fabric that such a said orbifold eigenset will be traveling through -- as it is to be moving with a relatively greater torque, than would otherwise be considered.  Consequently; let's consider an orbifold eigensest, that is here to tend to be moving naturally in its relative holomorphic direction. It is to bear a relatively greater torque per metric-gauge, than another comparative covariant orbifold eigenset.  The holomorphic-related drive in a direction or angular momentum-related wave-tug, of that inferred orbifold eigenset, that is here to work to bear a greater torque per metric-gauge, will tend to be of a higher scalar amplitude, than the holomorphic-related drive in a direction or angular momentum-related wave-tug, that would otherwise exist for the other inferred orbifold eigenset. Sincerely, Samuel David Roach.

As To Spatial Dimensionality And Velocity

Let's initially consider two different orbifold eigensets, that are here to be traveling at two different velocities, that are here to be covariant to one another.  One of these two said orbifold eigensets, is to be comprised of by superstrings of discrete energy permittivity, that are to bear a higher spatial dimensionality than the other said orbifold eigenset.  The orbifold eigenset that is here to bear a higher spatial dimensionality, is to also be traveling at a greater relativistic velocity than the other said orbifold eigenset.  This will then often cause the here mentioned orbifold eigenset, that is here to both be of a higher spatial dimensionality, as well as to be traveling at a greater scalar mangitude of a rate -- to not only tend to bear a greater pulsation, yet, this will often work to cause the faster orbifold eigenset of the two, to tend to bear a greater torque per metric-gauge that it is here to be applying upon its Hamiltonian operand.  Sam Roach.

Tangential Ebbing Of Superstringular Field Indices

The dual Ward-Cauchy-related process of the ebbing of convergent and divergent superstringular field indices, at the general region of the multiplicit core-field-density of the covariant proximal locus of individually taken superstrings of discrete energy permittivity, in the respective form of both an ebbing of the flow of hyperbolic cotangential mini-stringular segmentation, and, an ebbing of the flow of hyperbolic tangential mini-stringular segmentation -- works to help allow for the general ability of such said strings of discrete energy permittivity, to be able to vibrate, over the course of their iterative processes, in the substringular realm.  The closer that a Noether-based mass-bearing superstring of discrete energy permittivity is to be traveling, in its relationship to the motion of electromagnetic energy, the faster that such an inferred string is to tend to be able to vibrate during instanton. Sincerely, Samuel David Roach.

Tangential And Cotangential Flow

For any one particular superstring of discrete energy permittivity -- over the course of any given arbitrary iteration of group-related instanton, there is both a general genus of a hyperbolic tangential flow of mini-stringular segmentation emitted Outward from the core-field-density of the said string, And, a general genus of a hyperbolic cotangential flow of mini-stringular segmentation delineated Inward upon the core-field-density of the said string.  This eludes to the simultaneous mini-stringular ebbing of dual Ward-Cauchy-related conditions, (at the vantage-point of a central conipoint), of both a divergence of superstringular field indices that are brought Out of the core-field-density of such a respective given arbitrary string, And, a convergence of superstringular field indices that are brought Into the core-field-density of such a respective given arbitrary string. To Be Continued!  Sincerely, Samuel David Roach.

Hyperbolic Tangential Flow And Superstrings

The general tense of the multiplicit flow of mini-stringular segmentation, that is here to be emitted outward From the general core-field-density of the covariant proximal local region, in which a superstring of discrete energy permittivity is to be existent at, over the course of any particular iteration of BRST, -- is to be a general genus of a hyperbolic tangential flow.  Such a said general genus of a hyperbolic tangential flow, is to diverge From the multiplicit general core-field-density of a superstring of discrete energy permittivity, in a manner that is of a cross-product-based nature -- when this is taken in reference to the internal reference-frame, at the Poincare level, from the vantage-point of the here stated core-field-density of the said superstring. Sincerely, Samuel David Roach.

The Polyakov Action And Tangential Flow

The greater that the scalar magnitude of the Lorentz-Four-Contraction is to be, that is here to be applied to the topological stratum of a superstring of discrete energy permittivity -- the lower that the scalar magnitude of its directly corresponding Polyakov Action will tend to be.  The lower that the scalar magnitude of the Polyakov Action is to be, that is here to be applied to the topological stratum of a superstring of discrete energy permittivity -- the more of a scalar amplitude of a tense of consequential tangential flow, that will tend to be emitted from the proximal local core-field-density of such a said superstring of discrete energy permittivity.  I will continue with the suspense later! Sam Roach.

Some Stuff As To Conversion Of Mass Into Energy

When mass-bearing superstrings of discrete energy permittivity are to be converted into kinetic energy-related superstrings of discrete energy permittivity, -- such initially stated mass-bearing strings often tend to be opened up, at the covariant proximal loci of their directly corresponding partition-based discrepancies. I will continue with the suspense later!To Be Continued!Sincerely, Samuel Roach.

Stringular Spatial Dimensionality And Schwinger-Indices

The higher that the spatial dimensionality that is here to be exhibited, that is of any one given arbitrary superstring of discrete energy, the greater the potential variety of resultant Schwinger-Indices, that may tend to possibly be formed by the consequential "plucking" of the correlative second-order light-cone-gauge eigenstates, that are here to be of such a respective case, By the directly corresponding gauge-boson eigenstates, that are of such a respective correlative said inferred superstring of discrete energy permittivity. Samuel David Roach.  (PHS1989).

Some Stuff As To Space-Time-Fabric

Mini-Stringular Segmentation works to form those general fields, -- by which discrete energy and norm-state-projection-related commutation, are thence to be able to be held together, via what may be termed of here as being the general substringular condition of "homotopy." In-Between the countless eigenstates of mini-stringular segmentation, that are here to be existent in the substringular, -- there is the multiplicit proximal local presence, of what I term of here, as being the phenomenology of "pressurized vacuum."  The overall arena, by which the substringular is here to be exhibited by discrete energy -- over the course of the sequential series of the countless iterations of those instants, of what I term of as being the generally noticed durations of Ultimon Flow, there tends to generally  be the condition, by which such an arena is here to be filled by the summation of both the overall scalar magnitude of mini-stringular segmentation, Plus, the overall scalar magnitude of that pressurized vacuum, that is here to exist in-between the strand-like eigenstates of the said mini-stringular segmentation. I will continue with the suspense later! To Be Continued! Samuel David Roach.

Energy, Disturbance In Space, And Partition-Based Discrepancies

Energy tends to be produced by a disturbance in space-time-fabric.  Theoretically -- in general, in order for a bundle of discrete energy to exist (particularly, in order for a bundle of a multiplicit quantum of discrete energy permittivity to exist), its entity as an eigenstate of holonomic substrate-related phenomenology, as taken over the course of any one given arbitrary iteration of BRST, must tend to bear a topological surface, that may be mapped-out in a Laplacian-based context, in a manner that is piecewise continuous.  Yet, in order for the multiplicit eigenstate of a holonomic substrate of discrete energy permittivity to be able to move through a Lagrangian-based path, as an entitiy that may here be thought of in the context of being a Hamiltonian Operator that is here to be moving through the fabric of space and time, -- such a "thing" of discrete energy permittivity must consequently tend to be required to bear a tense of a disturbance in space, in order to actually bear the actual "motion" of discrete energy permittivity, -- in so as to work to allow for discrete energy to be able to move, so that it may both exist and persist as energy at all.  Consequently; there must be extremely mild aberrations from the Ward-Cauchy-related norm, of the general conditions of such earlier mentioned piecewise continuity, that is of the Laplacian-based state of a smooth contour, as taken along the topological surface of a superstring of discrete energy permititivty, in order for a superstring, that was initially formed by a disturbance in space and time, -- to then be able to move as a Lagrangian-related operator, so that discrete energy may be capable of actually acting as energy at all.  This is part of the reason, as to why there must be one or more partition-based discrepancies, which act as extremely mild aberrations that may be mapped-out, as taken along the contour of the outer perimeter of the holonomic substrate, that is of the topological surface of any superstring of discrete energy permittivity. Sam Roach.

Dimension Of Superstring And Wobble

The greater that the number of spatial dimensions is to be, of any one given arbitrary superstring of discrete energy permittivity -- as when taken over the course of any one given arbitrary respective iteration of BRST, -- the more of a relative scalar amplitude that such a said superstring of discrete energy permittivity will consequently tend to wobble by, when this is here to be considered over the course of a covariant iteration of group-related instanton. To Be Continued! Samuel David Roach.

Wave-Tug And Abelian Nature

Let's initially consider the wave-tug of a mappable trace of an eigenstate of mini-stringular segmentation, that is here to act as an eigenstate of a substringular related field.   The more relatively supplemental that the Yukawa-based action is to be implemented, in respect to the wave-tug that is here to be exhibited by such an eigenstate of mini-stringular segmentation, as taken over an evenly-gauged Hamiltonian eigenmetric in time and space, --- the more abelian that the consequentially resultant geometry of such an inferred tense of a wave-tug, may thence tend to be attributed to the said Yukawa-based action -- that is here to be applied by the eluded-to eigenstate of substringular field Upon the inferred holonomic substrate, that the said tense of mini-stringular segmentation is here to be acting upon in a kinematic manner, over time.  I will continue with the suspense later! Sincerely, Sam Roach.