Fortification Due To Oscillation-Based Tendencies

Just as the E(8)XE(8) Ward-Cauchy-related oscillation-based tendency operates, in so as to work to help at fortifying the structural integrity of their correlative orbifold eigensets -- the general action of E(6)XE(6) strings, in so as to work to form their pertinent correlative oscillation-based tendency among light-cone-gauge eigenstates -- works to help at fortifying the structural integrity, of those light-cone-gauge eigenstates, that work to form the discrete energy impedance of the directly corresponding orbifold eigensets, that are comprised of, in part, by these said light-cone-gauge eigenstates.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Eleventh Session Of Course Ten

When a second-ordered light-cone-gauge topology is plucked by a gauge-boson, the activity of such plucking is known of as a light-cone related gauge-metric, and, the vibration of such a gauge-metric is known of as a second-ordered Schwinger Index.  The individual mini-string links between a superstring and its associated Fadeev-Popov-Trace are known of as second-ordered light-cone-gauge eigenstates.  The whole general holonomic field topology of these links that exist in-between a superstring and its corresponding Fadeev-Popov-Trace is known of as a first-ordered light-cone-guage eigenstate.  The sum of the vibrations that are formed by a first-ordered light-cone-guage eigenstate is known of as a Schwinger Index (first-ordered).  A second-ordered Schinger-Index may be delineated through an arbitrary given Rarita Structure eigenstate with a tense of orphoganal Yakawa gauge activity, and thus bear a harmonic wave propagation along the said associated Rarita Structure eigenstate.  Or, a second-ordered Schwinger-Index may be delineated with a tense of assymetric multiplicit (in terms of directorals) Yakawa gauge activity, and thus bear an anharmonic wave propagation along the same general type of associated Rarita Structure eigenstate.  When a gauge-boson (E(6)XE(6)) that plucks a second-ordered light-cone-gauge eigenstate does not bear a tense of borne tangency in terms of the associated homotopic Ward directoralization -- the gauge-boson as a whole is not orphoganal as a unit upon the given second-ordered light-cone-gauge eigenstate, the said  E(6)XE(6) string that forms the perturbation here in the proximal locus of the given arbitrary Rarita Structure eigenstate causes an anharmonic wave metric-gauge that, in and of itself, tends to move in the direction of the course of propagating an eventual Wick Action.  A Wick Aciton is the most important form of a Hausendorf Projection.   

The Importance of the Interaction That Exists Between the Light-Cone-Gauge and the Rarita Structure

Each second-ordered light-cone-gauge eigenstate is plucked like a string of a harp to allow for vibrations known of as Schwinger Indices to propagate along the Rarita Structure in such a manner so that there is an interconnection in-between both discrete units of energy permittivity and discrete units of energy impedance with gravitational particles so that the amplitude of the Ricci Scalar may be, within reason, able to spontaneously allow gravity to take a certain degree of hold upon the basis of substringular interplay.  The phenomena that "plucks" the second-ordered-light-cone-gauge eigenstates are known of as gauge-bosons.  Gauge-Bosons are also termed of as E(6)XE(6) strings.  So, the harmonics and the anharmonics of the Schwinger Indices along the topological Fourier-Based trajectory of where the holonomic substance of the Rarita Structure is located at any given arbitrary sequential series of instantons in which the interaction of the said Rarita Structure upon gravitational particles bears a type of multiplicit gauge-metrical basis that causes gravity to be applied to discrete units of energy so that gravity may exist in the manner that it is applied to be is thus the phenomena activity that allows for the general basis of a type of amplitude known of as the Ricci Scalar.                                       
Just a little bit for now.
Sincerely,
Samuel David Roach.

More As To the Dangers of the Hadron Colliding Experiment

I have some knowledge that I would like to share as to why the Hadron Colliding Experiment should be shut down.

                
I have a blog entitled samsphysicsworld@blogspot.com. Within this blog, I have a post named the Leverage of the Higgs Action.

I also have commented on Linkedin about the dangers of the Hadron Collliding Experiment.

You can reach my blogcite via google. Please feel free to read any of my blog and comment about it if you wish!

My reasons for the acknowledgement of the dangers that I have mentioned above are fourfold:

1) The leverage of the Fischler-Suskind-Mechanism upon the Higgs Action as a scalar is the reciprical of the fraction of a Coulumb that forms discrete charge. (1/6.25*10^18)=1.6*10^(-19).

2) E(6)XE(6) strings that are adjacent spin assymetrically as a safeguard to homotopy -- and thus should not be collided together.

3) E(8)XE(8) strings that are adjacent spin assymetrically as a safeguard to homotopy -- and thus should not be collided together.

& 4) Gluons should not be collided together, because the gauge-metrical activity of gluons is the source of the Wick Action -- and undoing the Wick Action could "domino" fissures in space-time-fabric that could be detrimental to homotopy and thus detrimental to life.

Once you have rigorously considered the knowledge that I have presented to various people, please do all that you can with your standing in the global community to help end the Hadron Colliding Experiment.

Sincerely,





Sam.

The Danger of Colliding Two Photons Head On

• Hi, my name's Sam. As to the condition that would exist if you were to try to collide two photons dead on, that's a bad idea. Here, let me explain.


                   
Photons are formed by electrons dropping an energy level to release unneeded energy. When this happens, a Fujikawa Coupling happens in the direction of the permittivity of the a given photon, yet, in the reverse-holomorphic end of the bosonic superstring that forms a discrete unit of energy permittivity. Ward Norm conditions form the basis of substringular differential geometry. So, if you were to take the norm-to-holomorphic spin-orbital-axial of the delineation of the described Fujikawa Coupling as the photon is being formed from the released kinetic energy of a said electron, you get an orphogonal wave-tug upon the said photon that causes its related E(6)XE(6) strings to lay in the direction of the transversal angular momentum of the said photon. Also, if an electron is quantized at all with other photons, it is going to exist in an orbifold. Orbifolds have E(8)XE(8) strings associated with these. Remember, E(6)XE(6) strings that are adjacent spin assymetrically as well as E(8)XE(8) strings that are adjacent spin assymetrically. So, to try to smash the described heterotic superstrings is an effort to abuse the tendencies of these said heterotic strings to spin assymetrically. This is no mistake in observation, yet, doing what they are trying to do is certainly a mistake. Without the assymetric spin-orbiting of E(6)XE(6) strings, the Rarita Structure would be damaged locally -- which could lead to a "domino" effect. Without the assymetric spin-orbiting of E(8)XE(8) strings, the homotopy of adjacent orbifolds would fishure, which could have a "domino" effect. Maintaining homotopy is quintessential for the continued existence of life.

Also, colliding gluons could undo the local Wick Action eigenstates, which could have a domino effect. Please let everyone read this so that we may --- as a team -- end the Hadron Colliding Experiment. Thank You. Sincerely, Sam. Life is the most important reality.
                                                                                           

Some More Stough About Gauge-Bosons

Gauge-Bosons are essential in the field of a light-cone-gauge-eigenstate since, when individual gauge-bosons "pluck" the second-ordered light-cone-gauge-eigenstates that exist in the field of a first-ordered light-cone-gauge-eigentate, the resulting vibrations are second-ordered Schwinger Indices (the summation of such vibrations per first-ordered light-cone-gauge-eigenstate being a first-ordered Schwinger Index) that flow through the Rarita Structure to allow for the Ricci Scalar to function so that gravity may take effect. This is just in reference to the E(6)XE(6) type of gauge-bosons. Just as adjacent electrons have to spin assymmetrically, to give a reverse-fractored example, in order to obey the Pauli Exclusion Principle, adjacent E(6)XE(6) strings must bear an antisymmetric spin-orbital tensorism in order to not infringe on each others' space. Such an assymmetric spin-orbital tensorism is caused by the spurious effect of the Chern-Simmons field that exists between adjacent E(6)X(E(6) strings. Such a Chern-Simmons field is due to the condition of such gauge-bosons differentiating per instanton in-between a discrete energy unit of permittivity and a discrete energy unit of energy impedance. So, whether a related light-cone-gauge topology is abelian or non-abelian, the substringular field that binds these gauge-bosons to both sides of an associated first-ordered-light-cone-gauge-eigenstate is primarily abelian so that the "plucking" of the second-ordered light-cone-gauge-eigenstates will not shatter the given first-ordered light-cone-gauge-eigenstate. The fabric of substringular field is what I call "mini-string." Mini-String is the fabric of gauge-action that interconnects the topology of all unfrayed substringular phenomena that forms the homotopic structure of the substringular. My website is http://www.samsphysicsworld@blogspot.com.
          

Sincerely,

Samuel David Roach