Session 5 Of Course 20 -- Calabi Manifolds And Interactions

Light in a vacuum of space travels at 3.0*10^8 meters per second.  When light enters a medium that is not electromagnetic energy while it is also not a worm-hole, the light will tend to travel at a speed that is less than light speed.  For instance, when light strikes air, the light not only bends to a slight extent, it will also slow down to a correlative extent as well.  Once that light strikes the air, it will scatter -- while then subsequently tending to re-quantize to form light again.  Once the light reforms as light again, it will tend to travel in what amounts to as its given "tense of bend", yet in segmentations that are each of a relatively straight line, -- to where the said light, as it is here to be as is according to Snell's Law, is to then to go just slightly less than what light speed would be in a theoretical vacuum, as the so-eluded-to electromagnetic energy is to travel in the direction of "least time," as it is to only slow down and change direction, after each of such scatterings of the said light upon the so-eluded-to Calabi-Yau phenomenology of the said air molecules that it is to strike in a Gliosis-based manner over time.  For example, let's say that the given air was homogeneous in density, and that the light that I am referring to here did not have to significantly re-scatter again in the air, as the given light is here to be propagated downward toward the earth.  The light in this case is propagated towards the face of a body of water.  When the light strikes the water initially, the light will scatter, while then re-quantizing back into a beam of light that bends as is according to the density of the water -- and slows down as is according to this same density of the water.  The beam of light may be able to do this, if it is also not scattered by any plain kinetic energy, -- as other beams of light are to be inter-playing in this case scenario as well.  This beam of light may propagate until it is fully absorbed, most potentially by some alterior Calabi-Yau  space of mass.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Entropy And Cohomological Degeneration

Let us initially consider a photon of a beam of light, that is to strike an electron, that is of a set of atoms that are here to work to comprise a gauged overall mass-bearing phenomenology.  As the said photon is to strike the externalized core-field-density of a light-cone-gauge eigenstate of the electron that the so-stated photon is to collide with, in what is here to be in a Gliosis-based manner, -- that particular light-cone-gauge eigenstate of that discrete quantum of energy of the correlative electron that the said photon is to strike, -- is to initially -- upon its Gliosis-based collision with the said externalized core-field-density of the said light-cone-gauge eigenstate -- to become of an entropic-based manner, for an overall course of 384 consecutive iterations of group-related instantons, --in so long as the so-stated photon is not to collide with the externalized core-field-density of the holonomic substrate of any other light-cone-gauge eigenstate.  As the so-stated photon is to behave in an entropic-based manner, the said entropic photon is to tend to purely degenerate the cohomological stratum that it is to interact with, in a Yukawa-based manner.  Entropy never tends to bear the tense of being conformally invariant -- at the internal reference frame at which it is here to be operational chaotic or entropic in its behavior here.  An entropic condition is a condition of chaos or disorder.  Disorder or chaos is not of an organized manner, when the processes of such chaos is entropic or out of order or out of organization.  Disorder or chaos works to disorganize things.  Disorganization thus works to degenerate cohomological stratum, at the Ward-Cauchy level that is Poincare to the processes of its said disorganization.  Therefore, entropic photons are examples of photons that are here to be perturbated into a Rayleigh-based state of a scattering mode.  Entropic photons that are adjacent, will thus tend to bear an odd chirality-based parity -- over any correlative gauged group-metric that is of an even Hamiltonian operation.  Thus, the re-quantization of photons that were once entropic -- to where the said re-quantized photons are to then to return to a tense of working to bear a harmonic order -- is an example of a Reimman scattering, that is to bear photons that are no longer entropic in a discrete arrangement, in which the adjacent correlative eigenindices of the discrete electromagnetic quantum of energy are here to bear an even chirality-based parity.  (Now that such a discrete quantum of electromagnetic energy is to no longer be entropic.)  I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Orbifold Eigensets -- Different Reference Frames

Let us initially consider a set of superstrings, that operate in so as to form one specific function -- as what is here to be the eminent presence of one given arbitrary orbifold eigenset.  Let us consider that the respective orbifold eigenset of this case, is to bear a relatively high scalar amplitude of a tense of Majorana-Weyl-Invariance -- when this is taken at an internally-bearing of a Ward-Cauchy-based reference frame.  Next, let us say that the orbifold eigenset as a whole phenomenon, is to here to be moving in a transversal-based manner -- via a discrete unitary Lagrangian, in such a manner to where the scalar magnitude of the said orbifold eigenset's velocity, as it is traversing its so-eluded-to discrete unitary path, is here to be about cosine(30 degrees)*(the speed of light).  As the said orbifold eigenset is here to be traveling in a relatively "straight" manner at a rate of cosine(30 degrees)*(the speed of light), -- it is here to bear a Lorentz-Four-Contraction upon its internally composite set of superstrings -- that are here to work to make-up the so-stated orbifold eigenset, of a factor of two.  So, as those superstrings that are here to move in a tense of Noether Flow, as these discrete quanta of energy are here to be working to comprise the said orbifold eigenset, -- each of the superstrings of discrete energy permittivity that  work to help at forming the so-stated eigenset, are to then to bear a Lorentz-Four-Contraction of a factor of two. This would as well work to mean, that the here involved Polyakov Action that is to be directly correlative in this case, would then work to bear a scalar amplitude of a factor of 1.5*10^8.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.