Change Of Electrodynamic Flow And Chern-Simons Singularities

When an electrical current ( a tense of charge per time) is to bear a tense of perturbation, over a given arbitrary course of time -- this tends to be indicative of the directly corresponding presence of Lagrangian-based Chern-Simons singularities, -- as appertaining to the here correlative manner of the kinematic activity of the said electrical current.  Consequently; when amperage is to work to bear a tense of perturbation over time, this tends to be indicative of the presence of the directly corresponding presence of Lagrangian-based Chern-Simons singularities.  Furthermore; when the flow of the magnetic field is to bear a tense of perturbation, over a given arbitrary course of time, this tends to be indicative of the directly corresponding presence of metric-based Chern-Simons singularities.  Consequently; when a tense of voltage (a tense of energy per charge) is to bear a tense of perturbation, over a given arbitrary course of time -- this tends to be indicative of the directly corresponding presence of metric-based Chern-Simons singularities, -- as appertaining to the here correlative manner of the kinematic activity of the here inferred tense of energy per charge. I will continue the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Superstring Momentum And Isotropic Tendency

Any given arbitrary Noether-based superstring of discrete energy permittivity, that is of an isotropically stable nature -- will often tend to have a stronger attribute of angular momentum than spin-orbital momentum.  As a logical consequence; any given arbitrary Noether-based superstring of discrete energy permittivity, that is of an isotropically unstable nature, -- will often tend to have  a stronger attribute of spin-orbital momentum than angular momentum. Sincerely, Samuel Roach.

Fields And Chern-Simons Singularities

When there is to be an alteration in that fractal of the electric field, that is here to be directly associated with that motion of the Noether Current, that is here to be of a given arbitrary orbifold eigenset, this will often tend to be caused by a spontaneous alteration in the angular momentum, that is here to be directly corresponding to such a here stated orbifold eigenset, over time, -- to where this will consequently tend to result in the formation of a correlative set of one or more Lagrangian-based Chern-Simons singularities, that are thence to be formed at the moment of such a spontaneous alteration in the angular momentum of such a here mentioned orbifold eigenset.  Furthermore; when there is to be an alteration in that fractal of the magnetic field, that is here to be directly associated with the motion of the Noether Current, that is here to be of a given arbitrary orbifold eigenset, this will often tend to be caused by a spontaneous alteration in the spin-orbital momentum, that is here to be directly corresponding to such a here stated orbifold eigenset, over time, -- to where this will consequently tend to result in the formation of a correlative set of one ore more metric-based Chern-Simons singularities, that are thence to be formed at the moment of such a spontaneous alteration in the spin-orbital momentum of such a here mentioned orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.

Unstable Momentum And Chern-Simons Singularities

Often when an orbifold eigenset is to become unstable in its directly associated angular momentum, this will tend to result in such a stated orbifold eigenset to consequently work to bear a set of one or more Lagrangian-based Chern-Simons singularities.  Furthermore; often when an orbifold eigenset is to become unstable in its directly associated spin-orbital momentum, this will tend to result in such a stated orbifold eigenset to consequently work to bear a set of one or more metric-based Chern-Simons singularities.

As To Hermitian Lagrangian And Hermitian Metric

When an orbifold eigenset is to work to bear a continuous tense of angular momentum, this will often tend to consequently work to help in causing such a stated orbifold eigenset, -- to work to bear the characteristic of exhibiting a Lagrangian, that is of a hermitian nature.  Furthermore; when an orbifold eigenset is to work to bear a continuous tense of spin-orbital momentum, this will often tend to consequently work to help in causing such a stated orbifold eigenset, -- to work to bear the characteristic of exhibiting a metric, that is of a hermitian nature. To Be Continued! Sincerely, Samuel Roach.

Ricci Curvature And Isotropic Stability

When a superstring is said to work to bear a flat Ricci Curvature, -- such a said superstring will consequently always tend to be isotropically stable.  I will continue with the suspense later! Sam Roach.

Superstringular Impedance And The Light-Cone-Gauge

The higher the superstringular impedance is to be, the greater the directly corresponding Polyakov Action is thence to be exhibited, for the here directly pertinent superstrings of discrete energy permittivity. And; The greater the directly corresponding Polyakov Action is thence to be exhibited, for the here directly pertinent superstrings of discrete energy permittivity, the more hyperbolically arcing that the directly corresponding second-order light-cone-gauge eigenstates, that are here to be correlative to such a said superstring of discrete energy permittivity, are consequently thence to be.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Light-Cone-Gauge And Settlement Of Stringular Structure

The vibrational oscillations of any one given arbitrary overall first-order light-cone-gauge eigenstate, works to help in settling the Ward-Neumman-related structural conditions, that are of both such an eigenstate's directly corresponding superstring, and of its correlative counter string, -- over the course of an iteration of any one given Planck Instant.  I will continue with the suspense later!  Sincerely, Samuel David Roach.

Basic Forces Of Nature And The Light-Cone-Gauge

The basic fundamental forces of nature are created, in general, by the interaction of discrete energy with superstringular fields.  The holonomic substrate of superstringular fields, are comprised of both the phenomenology of mini-stringular segmentation, And, the Ward-Cauchy-related phenomenology of pressurized vacuum.  Mini-Stringular segmentation is perpetuated in its existence, by its general disturbance in space.  The general disturbance of space, which is here to work to help in the perpetuation of the existence of that multiplicit stratum of inferred stringular field, by which I am here referring to the continual general multiplicit existence of mini-stringular segmentation, -- is here to be mainly caused by the general propagation of the vibration of light-cone-gauge eigenstates (and light-cone-gauge eigenstates are the phenomenology of discrete energy impedance). This is to where such eigenstates, of which are here to be caused to vibrate, due to the resultant action of the "plucking" of  second-order light-cone-gauge eigenstates by gauge-boson eigenstates, is to happen, to where this is the main general means, by which the Rarita Structure is here to be perpetual in its continuation --- due to such a general activity of "plucking," to here be of a nature, by which to consequently work to cause the vibration of the multiplicit stratum of superstringular field.  The vibrational oscillation of such implied stringular fields, is thus to be able to spontaneously continue to exist indefinitely, due to the vibration of such here mentioned light-cone-gauge eigenstates.  Therefore; the main reason for the cause of such basic forces of physical nature, is the condition-related existence of the light-cone-gauge.  Thus; the existence of the light-cone-gauge, is the main reason for the perpetual existence of reality. Sam Roach.

Touching Base On A Past Idea

Just a reminder:

When one is here to be in the process of working to determine a tense of a genus of a superstringular-related knotting equation, when in reference to a symplectic cohomology, one is here, in part, to be mathematically converting a Minkowski Space into a Hilbert Space.  This is only just a small part of this inferred mathematical process.

When one is here to be in the process of working to determine a tense of a genus of a superstringular-related knotting equation, when in reference to a Khovanov (co)homology, one is here, in part, to be mathematically converting a Hilbert Space into a Minkowski Space.  This is only just a small part of this inferred mathematical process.

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Orbifold Eigensets And Scattering

When any given arbitrary orbifold eigenset is to disband into independent individually taken discrete quanta of energy, this is an example of one general type of a Rayleigh scattering.  Furthermore; when any given array of initially independent individually taken discrete quanta of energy are to come together -- in so as to become an orbifold eigenset, this is an example of one general type of a Riemann scattering. I will continue with the suspense later!  Sincerely, Samuel David Roach.

Adjacent Spinning Mass-Bearing Orbifold Eigensets

When two different adjacent given arbitrary mass-bearing orbifold eigensets, are here to be spinning at a relatively high rate -- these will each tend to need to bear a covariant asymmetric spin in relation to one another, -- in order to not infringe upon each other's space.  This is why adjacent electrons tend to bear a covariant asymmetric spin, in relation to one another, again, in so as to not infringe upon each other's space.  This specific general example that I just mentioned, in respect to the nature of the spin of adjacent electrons, is commonly known of as being the general gist of the "Pauli-Exclusion Principle."  I will continue the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cevita Interactions And Alteration Of Charge

When a given arbitrary Cox Ring, that is of one respective ordered grouping of a set of  cohomology-related eigenstates -- is to undergo a Cevita Interaction at the Poincare level, -- this general course of action, will tend to reverse-fractal into a tendency of working to cause the directly corresponding orbifold eigenset, that is here to be associated with the reverse-fractal of such an initially stated Cox Ring, to consequently work to bear an increased probability of spontaneously altering in the general tense of its correlative physical charge. I will continue with the suspense later!  To Be Continued!  Sam Roach.

Type Of Chern-Simons Invariants And Charge

The quicker that a mass-bearing orbifold eigenset is to fluctuate in its pulsation over time, -- the faster that the rate of its directly corresponding metric-related Chern-Simons Invariants will tend to fluctuate -- of which will consequently tend to reverse-fractal into resulting, in an increased scalar magnitude of charge per time, -- of which will then tend to result in an increased amperage.  The quicker that a mass-bearing orbifold eigenset is to fluctuate in the externalized distribution of its cohomology-related generation over time, -- the faster that the rate of its directly corresponding Lagrangian-related Chern-Simons Invariants will tend to fluctuate -- of which will consequently tend to reverse-fractal into resulting in an increased scalar magnitude of energy per charge, of which will then tend to result in an increased voltage. Sam Roach.

In Reference To Holomorphic Direction

Let us initially consider a superstring of discrete energy permittivity. Let us now say, that such a said string is to be facing -- in a Laplacian-related manner, towards the relative forward-holomorphic direction. Let's say that one is then to theoretically consider a Laplacian-related pivoting of the mentioned string, as a whole entity, by 90 overall degrees into the forward-holomorphic direction, to where the said string of such a given arbitrary case, is now to be facing, what was initially to be in its relative reverse-norm-to-holomorphic direction. (One is here to consider the relative "bottom" of the said string, to be at a fixed general locus.) Next; let's say that one were, instead, to consider a Laplacian-related pivoting of the said string, as a whole entity, by 45 overall degrees into the relative forward-holomorphic direction, from its initially stated positioning mentioned at the start of the given arbitrary scenario of this post. Let's say here, that the Initially inferred Holomorphic direction of this said given arbitrary superstring, is to be taken as to be of the general "i" direction. Consequently; once that the said string has been determined to have a Laplacian-related pivoting, as a whole, by 45 overall degrees, into the forward-holomorphic direction from its initial positioning, -- instead of the Norm-To-Holomorphic positioning of such a string to be facing in the relative (i-1) direction, -- instead, at this point in re-arrangement, the norm-to-holomorphic positioning of such a string, is now to be facing in the relative (((i-3)*(2^.5))/2) direction.  Consequently; at this point in consideration, the Reverse-Norm-To-Holomorphic positioning of such a string, is now to be facing in the relative (((3-i)*(2^.5))/2) direction (instead of it facing in its initially existent (1-i) direction.)  I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.

Back-And-Forth Of Fading Of A Tense Of Pressurized Vacuum

When any given arbitrary discrete increment of mini-stringular segmentation, is to be re-distributed by one discrete increment of spatial translation, from one positional delineation to another, -- it is to fade in and out of a tense of substringular pressurized vacuum, at an extremely rapid rate.  Here's what I mean by that.  A bead of mini-stringular segmentation (one discrete increment of "zero-point-energy"), is to be spatially translated via an externally applied wave-tug, through a sub-metric-related scalar distance, that is tantamount to the magnitude of the cross-sectional thickness of a generally normal segment of mini-stringular fabric.  The kinematic action of such an inferred externally applied wave-tug, that is here to act, in so as to re-distribute the said discrete increment of zero-point-energy, -- is to initially work to Temporarily (over an extremely infinitesimal duration) convert the said discrete increment of segmentation, into briefly existing as a tense of a tugged-upon "entity" of pressurized vacuum.  Consequently; as an equal and opposite reaction, that is happening from the opposite general direction -- since this temporary tense of pressurized vacuum is being tugged-upon, by the multifarious external Ward-Cauchy-related activities -- this multiplicit general action, will then almost always tend to work to immediately convert the "tugged-upon" pressurized vacuum, to go back into existing as a bead of mini-stringular segmentation, or, in other words, this will consequently tend to result in such said "tugged-upon" pressurized vacuum, to thereby re-convert back into being a discrete increment of "zero-point-energy." Samuel David Roach.

A General Genus Of An Isometric Covariant Yukawa Coupling

When a physical charge is to work to bear a Yukawa Coupling with a force-field, -- in a manner that is isometric in covariance, such a general genus of an interaction, is to tend to consequently work to form a certain amount of an electrostatic discharge, -- which is here to consequently tend to work to form at least a small amount of resultant electricity. Electricity is a flow of electrons.  Electrons bear mass.  Consequently; when a charge is to interact with a force-field in the particular general manner that I have described, this will tend to form at least a small amount of an electrostatic tense of mass. Sam Roach.

Discrete Segment Of Mini-Stringular Segmentation

One discrete segment of mini-stringular segmentation, is basically existent as a "bead" of such mentioned segmentation, -- of which is here to be on the order of behaving like that general phenomenology, that I have termed of here as being the Laplacian-related presence of a second-order point particle (with a relatively infinitesimal Laplacian-related presence, of what I term of as being "sub-mini-string," being subtended at either side of such an exhibited "second-order point particle.")  To Be Continued! Sincerely, Samuel David Roach.

The Smallest Holonomic Substrate

The smallest discrete "quantum" of a holonomic substrate that is not frayed -- that may be "divvied-out," is on the order of about 2.062365054*10^(-129)*6.62607004*10^(-34)Joules*Seconds, or, in other words, about 1.366538*10^(-162)Joules*Seconds. This would thence be equivalent, to the smallest "quantum" of mini-stringular segmentation that is not frayed, that may be translated via a duration, through any sort of a viable spatial delineation.  I will continue with the suspense later! Samuel David Roach.

What I Mean By "metric-gauge eigenstate" Versus "Metric-Gauge-Related-Field-Operator"

When I refer to the general Main Influence of physical nature, that is formed by the force of pressurized vacuum -- this influence of which is generally in terms of discrete increments of (energy of minimal mass equivalence, in Kg) /(minimal charge equivalence) -- I would say that this said influence should be denoted as being termed of as a "force-field" or a "Metric-Gauge-Related-Field-Operator", whereas, when I refer to a functioning substringular entity, that happens to be smaller than a superstring, I would say that this should be denoted as being termed of as a "metric-gauge eigenstate."  This is the manner that I personally feel would be fitting, to distinguish between these two distinctly different concepts.  Again, sorry for the confusion earlier.  Sincerely, Samuel David Roach.

Some Stuff About Change In Gravitational Mode

When the mode of gravity, that is here to be applied upon a Ward-Cauchy-related region, -- is to convert from a tense of a gravity to a tense of anti gravity or vice-versa -- this will tend to invert a tense of the sinusoidal conditions of those "quantized" gravity-related Schwinger-Indices, that are here to work to form such an altered mode of gravitational influence, that is here to have been changed from within such a stated Ward-Cauchy-related region in time and space. Samuel Roach.

Optimum Scalar Amplitude Of Angular Momentum

The closer that any given arbitrary Noether-based orbifold eigenset, is to approach a spatial translation of motion through a Lagrangian-based path -- that is here to be delineated into the relative forward-holomorphic direction, -- the more optimum that the directly corresponding scalar amplitude of its angular momentum, will consequently tend to be.  I will continue with the suspense later! Samuel Roach.

Orbifold Eigenstate Pulsation And Rate Of Transference

The quicker that any given arbitrary orbifold eigenstate is transferred in its delineation through space over time, the quicker that its rate of pulsation will consequently tend to be.  Next; let's consider two different orbifold eigenstates, that are both to be pulsating at the same covariant rate. Next; let's theoretically consider, in this particular case, that both of the here stated orbifold eigensets, are to be effected by the same scalar amplitude of substringular pressurized vacuum. Let's next say, that the individually taken superstrings of discrete energy permittivity, that work to comprise one of these two said orbifold eigensets, are to be vibrating at a quicker rate, -- than the individually taken superstrings of discrete energy permittivity, that work to comprise the other of the two said orbifold eigensets.  Let's next say, that both of these here stated orbifold eigensets, are to work to bear both the same number of superstrings of discrete energy permittivity, over the course of their spatial transference of delineation. Both of such here mentioned orbifold eigensets, are also to work to bear the same density. The orbifold eigenset of this particular case, that is here to work to bear the proximal local presence of those inferred superstrings of discrete energy permittivity, that are here to be vibrating at a quicker rate, -- will consequently tend to bear a greater fractal modulus -- than the other of the two mentioned orbifold eigensets. Sam Roach.

Substringular Pressurized Vacuum And Elastic Modulus

The higher that the scalar amplitude of the substringular pressurized vacuum is to be, that is here to be applied upon any one proximal local set configuration of mini-stringular segmentation, -- the lower that the correlative elastic modulus will tend to be -- of the directly corresponding said proximal local set configuration of mini-stringular segmentation.  Consequently; the lower that the scalar amplitude of the substringular pressurized vacuum is to be, that is here to be applied upon any one proximal local set configuration of mini-stringular segmentation, -- the greater that the correlative elastic modulus will tend to be -- of the directly corresponding said proximal local set configuration of mini-stringular segmentation.  To Be Continued! Sincerely, Samuel David Roach.

Rigidity Of Torsion Applied To Mini-Stringular Segmentation

The higher that the scalar amplitude of the substringular pressurized vacuum, that is here to be applied upon a relatively proximal local holonomic configuration of mini-stringular segmentation -- as this is here to be taken over an evenly-gauged Hamiltonian eigenmetric, -- the Greater that the the scalar amplitude will tend to be, of the rigidity of torsion, that will consequently tend to be applied upon the holonomic substrate of such a configuration of mini-stringular segmentation.  Consequently; the lower that the scalar amplitude of substringular pressurized vacuum, that is here to be applied upon a relatively proximal local holonomic configuration of mini-stringular segmentation -- as this is here to be taken over an evenly-gauged Hamiltonian eigenmetric, -- the Lower that the scalar amplitude will tend to be, of the rigidity of torsion, that will consequently tend to be applied upon the holonomic substrate of such a configuration of mini-stringualr segmentation. Samuel David Roach.

A Balance, Working To Help Form Steady-State

When an orbifold eigenset is to be undergoing a tense of superconformal invariance, there will tend to be a proximal local balance, --  between the kinematic activity of the Poisson-related functioning of such an eigenset, And, the kinematic activity of the Green-related functioning of such an eigenset, that is here to be most associated with the covariant flow of the delineation of those discrete quanta of energy, that are here to work to comprise such an inferred set of discrete quanta of energy, that operate to perform one specific task -- to where such a "team" of discrete energy, that are here to work to make-up this holonomic substrate, will consequently tend to be of a mass-bearing topological-related stratum. This is a reverse-fractal, of what one would normally think of as being of a steady-state scenario.  Samuel Roach.

As To Forward-Magnetism And Reverse-Magnetism

Thought waves that are theoretically solely influenced by forward-magnetism, tend to be more susceptible to being Ward-Polarized by gravity, whereas; thought waves that are theoretically solely influenced by reverse-magnetism, tend to be more susceptible to being Ward-Polarized by anti gravity.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Coupling Of Gravity Waves And Thought Waves

Both individually taken gravity waves and thought waves that are of the same scalar magnitude of wave-length, tend to be of a covariant relationship, that is of a potentially Ward-Polarized nature.  Therefore; when a thought wave and a gravity wave that are of the same scalar magnitude of wave-length are to couple in a directoral-related manner, this will often tend to form a resultant transference of a tense of energy, -- that will tend to bear a flow in the direction of the relative mean Lagrangian -- when this is here to be taken in retrospect to the initial flow of both the individually taken gravity wave and the individually taken thought wave, that is here of such a given arbitrary case. Sam Roach.

Alteration In Hyperbolic-Related Gravitational Sway

Let us theoretically consider a physical entity of mass, that is initially here to bear a hyperbolic-related sway in its Lagrangian-based pah, that is solely due to the influence of anti gravity.
Let us next say, that there is then to be an instantaneous change, -- that is then to work to cause this originally stated given arbitrary respective physical entity of mass, to go into working to bear a hyperbolic-related sway in its Lagrangian-based path, -- that is solely due to the influence of gravity.  This general process, will consequently work to cause a definite tendency, -- of resulting in both a set of Lagrangian-related Chern-Simons singularities As Well As resulting in a set of metric-related Chern-Simons singularities, -- at the locus in which there is here to be the inferred instantaneous alteration in the general tense of gravity, that is here to be physically applied to the initially stated physical entity in time and space -- that is here to consequently tend to both alter in its general tense of hyperbolic concavity, as well as simultaneously (via the vantage-point of a central conipoint) to tend to alter in its dimensional-related pulsation. (This is to where, such a general activity will tend to work to cause an inversion in the general tense of the augmentation/attenuation of its initial torsion, upon its holomorphic state of pulsation.)  To Be Continued!  Sincerely, Samuel David Roach.

Reiterating Why I Feel CERN Should Be Cautious

Discrete charge is About 1.6*10^(-19) of one coulumb.
The Leverage of the Fischler-Suskind Mechanism, upon the multiplicit holonomic substrate of the (multiplicit) Klein Bottle -- in so as to work to move the multiplicit Higgs Boson eigenstate into its main function, is on the order of About 6.25*10^(18).
The number "1.6*10^(-19)" is the reciprocal of the number "6.25*10^(18)."
Based on this general type of a consideration, -- isolating an eigenstate of the Higgs Boson , may potentially work to undue, at least a small degree of discrete charge -- in an unwarranted manner, to where this may potentially cause an unwanted fissure in space and time, -- to where this could possibly work to form a black-hole.  Black-Holes Should Not Be Harnessed.  These work to fray substringular phenomenology, of which is then to be subsequently "spit-out" at a different general locus as anti matter -- of which is then to subsequently to go into the process of re-organizing into matter.  This is why those general activities of CERN, -- in which such a process of doing such things like "isolating the Higgs Boson," should be refrained from, if you are able to "see what I mean."
"NOUS SOMMES ICI!"

I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Another Way Of Looking At The "Potentially Viable Idea"

Consider the following; then, see what you think of this:

Take:  (((The smallest discrete transversal-related "quantum" of that main influence, that is produced by the thought force)
 *(The smallest discrete transversal-related "quantum" of that main influence, that is produced by the force of pressurized vacuum)
*(The smallest discrete transversal-related "quantum" of that main influence, that is produced by the point commutative force)
*(The smallest discrete transversal-related "quantum" of that main influence, that is formed by the electromotive force)
*(The smallest discrete transversal-related "quantum" of that main influence, that is formed by the gravitational force)
*(The smallest discrete transversal-related "quantum" of that main influence, that is formed by the weak force)
*(4.135607315*10^(-17) of one Watt))
ALL / (The smallest discrete transversal-related "quantum" of that main influence, that is formed by the strong force))

=

The main mathematical expression of scalar magnitude, that is used to describe the energy*time of the transversal characteristic of one "strand" of mini-stringular segmentation, -- to where this here to be related to the concept of "zero-point energy."

(`2.062365054*10^(-129)*(6.62607004*10^(-34) of one Joules*Seconds), or, in other words, this is 2.062365054*10^(-129) of the Planck Constant!
Sorry for the mistake about this earlier!

To Be Continued!  Sincerely, Samuel David Roach.