Course 3 on Lorentz-Four-Contractions, Session 15, Part 1

Think of an object. It contains strings that are distributed throughout all 32 dimensions of the set of parallel universes that it is in. Some of the said strings cut through all 32of the dimensions. Some of the strings only exist in one dimension. The strings of the given object are thus arbitrarily assorted within any parameters which include directorals that fall in the dimensional fields that exist within the Continuum at that general region. Say, for instance, that the object given is not moving in an exact given dimension that we would call "forward holomorphically", "side-to-side", or "up-and-down." Let us think that a tangential motion relative to the earth was considered as a: Directoral axis (thickness of earth) based on a three-dimensional axes that included an earth associated axis that is tangential to it; associated, while the axis going "up-and-down" would arbitrarily be the k directoral. Let us arbitrarily define the dimensional situation and placement of the strings of the object based on the given directorals and the other 29 dimensions that one may define based upon the proscribed assortment of the directoral indices that we have shown. Make the axial size down to the discrete level of the width of a string, and the length of the axes as to include the field that defines the scope of the total range of motion of the given object. The object moves within its Ward boundaries. It does not move parallel to any of the given axes. It moves, say, in an arch that falls within the fields of each of the dimensions of the axes that define the region where the object moves. Since the object is always changing direction, it is constantly accelerating. I will conclude this session so as to relieve your suspense at a later time. I'm hoping that you can picture what I am describing in detail. If you can see a concept in your mind, the solution is clear.
Sincerely,
Samuel David Roach.

More About Photon Formation

When a fermionic superstring of an electron has its Campbell indices of its field generation struck, it alters to form a bosonic superstring. As the superstring discussed has its field projection struck, the one-dimensional superstring discussed will torsion initially to allign in the direction that it is to scatter in. In the time or metric between two successive Kaeler metrics, the associated one-dimensional superstring aligns in its direction as its Campbell field indices are struck to allow the reverse holomorphic direction of where the superstring is to scatter to begin the Fujikaws coupling discussed. The holomorphic direction of where the superstring is to scatter is where the light-cone-gauge eigenstate associated is directoralized as a gauge-action. The one-dimensional superstring initially realigns to form the directoralization where it is to scatter, while then scattering outward to form a two-dimensional superstring via the Green function via a Yakawa coupling known as a Fujikawa coupling. This here will involve two immediately successive gauge transformations, which are examples of two successive Gaussian Transformations. The aligning of the associated Campbell projected field of the one-dimensional superstring that will form a two-dimensional superstring will alter the physical norm conditions of a locus of superstrings. This "backgammoning" is what forms a Gaussian transformations here. The difference between a gauge transformation and another Gaussian transformation is that gauge transformations always involve entropy, seeing that Kaluza-Klein topology always involves entropy. If the light-cone-gauge topology is maintained, the Gaussian transformation is not gauge.

GUFT, Another Addition

The Klein bottle exists for the purpose of Kaeler metrics. The Kaeler metric is the gauga-metric sequential series that allows for superstrings to shake back and forth thru a series of 191 iterations or instantons eight timers per iteration so that a set of superstrings per Klein bottle per utilization may regain the permittivity that these need so that these associated superstrings may be the energy that these are to be. Superstrings are the permittivity of discrete units of basic Planck energy. The Kaeler metric also causes the field trajectory of superstrings which are known as Fadeev-Popov-Traces to reatain the impedance that these need so that these may secure the energy of the superstrings so that discrete energy may not form an imaginary supercharge that would destroy everything. So, the Fadeev-Popov-Traces act as the impedance of discrete units of energy. The Klein bottle is lifted toward the locus of where the Kaeler metric is to happen via a particle known as a Higgs Action.The Higgs Action is moved via an operation (Fourier) known as a Fischler-Suskind mechanism. The Fischler-Suskind mechanism is a leverage operation that increments the Higgs Action one Planck Length at a time via a gauge-action known as a Landau-Gisner Action. The Landau-Gisner Action is triggered by a Hausendorf Projection known as a Wick Action. The Wick Action is formed by the alteration or perturbation in the norm conditions (Ward normal) of the superstrings and the norm Ward conditions of the orbifolds and the norm Ward conditions of the torroidal cohomologies of the superstrings of the orbifolds of an orbifold eigenset that cause a substringular profection per associated Klein bottle locus that appertains to the need for a Gaussian Transformation. The Klein bottle is built in a fashion known as a Schotky Construction. A Schotky Coonstruction is comprised as follows: It has five sides with no relative "top" in the form of a half-cube that is empty of superstrings and has no cap. It has sides that are the thickness of the Planck Length with norm states inside of it that are Campbell indices that here are negative norm statess. The four sides that arae parallel are known as orientifolds. The Schotky Construction of the Klein bottle'ss norm indices and angled at 22.5 degrees from each other subtended back-and-forth from layer of states to layer of states. This low pressure in the Klein bottle gives it a low substringular pressure that makes it have a norm to reverse/norm to forward holomorphic pull that is based on the Minkowski Hodge Index of one of its walls. The overall push on the Klein bottle thus allows it to be moved "upward" by the forces acting thru the Higgs Action via the Higgs Action. (A volume of third-ordered-point-particles with a leverage that has a backing has a greater Hodge Index than a relatively small Minkowski surface.) The Klein bottle or Schotky Construction rock-sways at 45 degrees 3-D subtended lengthwise by 22.5 degrees subtended widthwise per iteration as it reaches the plane where the superstrings are to enter it. (22.5 degrees subtended from the bottom of the Higgs Action holomorphically, then antiholomorphically.) The Higgs Action angles as described before for side motion of the Klein bottle. The superstrings then receive the Kaeler metric once per iteration for 191 straight iterations.