More 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-eigenstate, 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 antisymmetrically, 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 antisymmetric 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

Course 4 On The Substringular Vs. The Globally Distinguishable, Session 16, Last Test

1) What is the substringular?

2) What is the gloabally distinguishable?

3) How does phenomena differentiate relative to make the substringular appear as the globally distinguishable?

4) How fast does phenomena "circle" the ultimon?

5) Why is most physical phenomena a vacuum at any given moment?

6) When is a string a string? Describe an instanton.

7) How do point particles find heir way back to form a specific string?

8) How does spin effect the relationship between the subsringular and the globally distinguishable?

9) How does roll effect the relationship between the substringular and the globally distinguishable?

10) Describe point reformation.

11) How does point reformation effect he relationship between the substringular and the globally distinguishable?

12) Describe how point particles may form a vacuum when altered.

13) Describe how a vacuum may change into strings.

14) How does the multiaxial codifferentiation of a supersting effect its relationship to light.

15) Why must the multiaxial codifferentiation of a string be fully normalized in order for the associated superstring to be tachyonic?

16) When may a particle "catch up" with light?

17) Is the multiaxial codifferentiation of a "normal" superstring normal to or parallel with the general flow of point particles? Why?

Course 4 on The Globally Distinguishable Vs. The Substringular, Session 14, Part One

So, nuclei particles and electrons are composed of smaller particles. These smaller particles in the subsringular are actually sequences of strings that exist in individual parts of a tori sector. As these sequences iterate and reiterate, these effect the stuff that they interact with. These sequences also have direct wave connections with other of "such types" of sequences. Simplify to two stringular sequences. These are connected by wave during one quaternionic-instanton-field-impulse-range. Once the strings of these sequences leave the range of the instanton field, the point particles associated with these strings move out of a line formation and into a more scrambled formation. There is still at least some wave connection between some of the waves that existed not only between the points of the individual strings, yet also between the points of each string toward each other. As a matter of fact, if these strings end up reiterating in the same general relative locant, there will be some wave connection between all of the points of both strings during the whole transit of the strings as points around the Continuum. Not only will the condensed oscillations or points effect the stuff that it goes through, yet the strung out waves will also effect the stuff that these encounter on their way around the ultimon (Continuum). As a matter of fact, points have fields, as said before. Two things con not occupy the same spot at the same time. So, points tend to rely on strung out waves, in the substringular, to produce effects. I will continue with the suspense of this session later. Until then, have a phenomenal day!
Sincerely,
Sam.

Course 3 on Lorentz-Four-Contractions, Session 14, Part 2

Everything that exists down to a point particle within a point particle (a third-ordered point particle) differentiates when you examine these things within the substringular. Phenomena below the stringular level are not kinematic in terms of showing what we would call energy in the globally distinguishable or in the substringular. Each time a string as a globally "stationary" phenomenon reattains its position at the given locant or neighborhood that defines its relative position towards the other strings that comprise its conformally invariant environment, that string has then reiterated. Since everything changes, this includes stringular environments in both the globally distinguishable and the substringular. So even if a string was encoded to return to the same spot after successive iterations, that string may need to adapt and return to a slightly different spot that exists in the neighborhood of the prior iteration. This inevitably happens, since all points iterate within short periods. So, when an object is motionless, and it's temperature is just over 0 Kelvin (-273.15 degrees centigrade), the strings may not vibrate relatively much in the globally distinguishable. The substringular would continue to reiterate at the approximate relative position in so long as there is no additive change in the object. So, when one detects something, the detection takes time. Time involves the differentiation of light. Light involves the Planck Moment. During the Planck Moment, a string is reiterated once within a proximal neighborhood (a relatively local substringular range.) I will conclude Session 14 later. I am trying to convey things starting with ideas that are not overwhelming. If you have any comments or questions, please let me know. Until later, have a fantastic day.
Sincerely,
Samuel David Roach

Grand Unified Field Theory, Session 3

A ghost anomaly is a physical memory of either a superstring, a light-cone-gauge eigenstate, a Fadeev-Popov-Trace, a graviton or a gravitino, or a world-sheet. A ghost anomaly has both physical and non-physical states. A single physical ghost anommalic state of a Fadeev-Popov-Trace is known as a negative-norm state. A negative-norm-state, if it is a Campbell norm state, consists of a first-ordered-point-particle that is supplementally norm to a relatively few other first-ordered point particles when this state as a unit travels in the reverse holomorphic direction. An antiholomorphic state moves to the right relative to the left moving ultimon substringular flow. So, the positive time-bearing ultimon flow spins counterclockwise, while negative-norm-states traveling in this flow spin clockwise. As a superstring differentiates kinetically per iteration, it produces ghost anomalies per iteration. These ghosts in this case are physical states that differentiate in a position-like manner. As these ghosts accumulate, the Gaussian form of the orbifold of the given substringular field "feels" the pressure of these ghost anomalies. If there is not to be a Gaussian Transformation of the topology of the given orbifold, then the Landau-Gisner-Action will not be activated in the locus of that given orbifold.
The leverage of this pressure will pull positive-norm-states of the region of the orbifolds neighborhood that are off of the Real Reimmanian plane into the field of the negative-norm-states that have quantized to form the ghost anommalic region that is formed by the physical memory of the given superstring in question. As the superstring given continues to differentiate kinematically, the physical actions of the given superstring forms a world-sheet that is comprised of physical ghost anomalies that harbor in integrated quantum space. The positive-norm-states then scatter the negative-norm-states by striking at a 45 degree/(22 and a half degrees) subtended from straight rock-sway. This scatter also happens to the ghosts formed by light-cone-gauge eigenstates. The rock-sway is a twist of a positive-norm-state from the conicenter of its front of (22 and 1/2 degrees) subtended from the holomorphic "left" (relative to the front of the given norm state) to (22 1/2) degrees subtended from the relative holomorphic "right" of that given norm-state as the norm state moves to strike a norm-state at 45 degrees or at 135 degrees as subtended from a straight supplemental angle, depending on which side of the subtending that you are measuring from. A non-physical memory would be a morphological vacuum of substringular phenomena that helped indicate the past motion of certain substringular phenomena.