As To Torsion Acting Upon Superstring -- Light-Cone-Gauge Eigenstate

 Whenever a gauged-action, that is here to behave as a torsional force, is here to be imparted, upon a given arbitrary correlative superstring of discrete energy permittivity, -- this general genus of a gauged-action, will consequently tend to work to form a tense of twisting, upon its correlative directly corresponding respective light-cone-gauge eigenstate. I will continue with the suspense later! Be Continued! Sincerely, Samuel David Roach.    

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

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

Part Two of Session 8 of Course Nine

Each individual light-cone-gauge eigenstate has 44 angular momentum components, 84 orbital components, and 128 spin components.  This is due to the condition that, for relatively time-oriented supertrings, it is most basic for a light-cone-gauge eigenstate to rotate along its axial plane over the course of sequential instantons, while it is a little less basic for a light-cone-gauge eigenstate to rotate along a radial Lagrangian while yet maintaining a directly covariant association with a specific conipoint of the coniaxial that is related to an arbitrary superstring when it is undergoing a state of conformal invariance, while it is less basic, yet essential, for a superstring to undergo a perturbation in the locus of its coniaxial.  (Although Gaussian Transformation happen all of the time, because of intertia, it takes an outward force to transversally move a supersting out of conformal invariane in such a manner so as to allow for the continued flow of the countless Fourier Transformations that are associated with the kinematic interplay that allows space-time-fabric to spontaneously continue to exist.)  In one-dimensional strings, the 44 angular momentum components are excentuated beyond the other components, do to the condition that one-dimensional superstrings comprise the existence of plain kinetic energy.  In two-dimensional superstrings associated with the upper Royal Arc section, spin-related components are excentuated beyond the other components.  One-Dimensional superstrings have relatively timeless light-cone-gauge eigenstates -- partially on account of the condition that a one-dimensional superstring has a purely Minkowsk field that is directly associated with it.  (A one-dimensional superstring directly associates with a two-dimensional field.)  Two-Dimensional superstrings have relatively time-oriented light-cone-gauge eigenstates, partially on account that the three-dimensional fields that directly accomedate the respective two-dimensional superstrings, at least, bear some basis with a Hilbert-like field.  (Hilbert-based fields may have as little as three spatial dimensions associated with these.)  Yes, Minkowski space may have up to 26 spatial dimensions under the conditions of an arbitrary Laplacian setting, yet, the foundation of Minkowski space is two-dimensional space -- the basis of flat space is a planar two-diimensional field.  Hilbert space is volume-oriented space.  Hilbert space may be comprised of as little as three spatial dimensions under certain conditions.  Time-Oriented light-cone-gauge eigenstates, which, are of two-dimensional superstrings,  have ten second-ordered light-cone-gauge eigenstates that comprise the initially mentioned first-ordered light-cone-gauge eigenstates of the described two-dimensional superstrings.  Relatively timeless light-cone-gauge eigenstates exist in the field of one-Dimensional superstrings, these of which have five second-ordered light-cone-gauge eigenstates that comprise the initially mentioned first-ordered light cone-gauge eigenstates that are associated with the described one-dimensional superstrings.  Two-Dimensional superstrings are closed, while one-dimensional superstrings are open.  Most superstrings have bear light-cone-gauge eigenstates that are relatively time oriented, so, most superstrings are closed , or, in other words, most superstrings are bosonic.  Yet, fermionic or open superstrings must exist.  If open superstrings did not exist, a photon would implode as it was formed, yet, thank goodness for the fact that their is plain kinetic energy (it is a fact of reality), so as long as there is a Continuum, there will be a certain arbitrary amount of one-dimensional (fermionic) or open superstrings.  I will continue with the suspense later!    I have a couple more posts to do on this session to ellaborate further as to the meaning of what I have been describing here.Until then, move closer and closer to your goals, and you will move in the direction of which you think!  Sincerely, Sam 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.