A Certain Aside As To Assymptotes

Let us consider an orbifold eigenset, that is moving into the general reverse-holomorphic direction -- in an assymptotic directorial-based manner, towards a plotting that may be mapped-out as being of a general relative y-based axion, -- to where this happens in such a manner, that may be described of as a cohomological index, that behaves as if it is moving as an eigenstate that is as well moving in a tangential manner, via a respective correlative Fourier-Transformation, that is initially being translated via an even manner of acceleration, over time.  Let us initially consider that one is dealing with a "real-to-'life'" relatively planar motion (as a figure of "speech"), that is basically moving in a strictly two-dimensional manner, as the said orbifold eigenset is to approach the so-stated relative y-based axion, in an assymptotic manner, over a sequential series of instantons.  Let us next consider, that at some point in time -- as the said orbifold eigenset is to then be relatively very close in proximal locus to the said mapped-out relative y-based axion, -- that the so-stated orbifold eigenset, that is to here be kinematic in displacement, via the so-eluded-to Fourier-Transformation, is to be tugged-across the Laplacian-based mapped-out y-based axion.  Since this general genus of a perturbation out of the initial assymptotic mode of motion, will be an alteration out of the general genus of the so-eluded-to approach -- that had initially been tending to get nearer and nearer to the plotted-out relative respective y-based axion -- in such a manner of which is to here be moving as is according to the so-stated initial even acceleration, over the initial so-eluded-to sequential series of instantons,  such a perturbation out of an assymptotic flow of the respective eigenindices of the said orbifold eigenset, will blatently work to cause a change in the initial rate of the acceleration of the said orbifold eigenset, -- to where such a genus of a kinematic-based perturbation will then work to cause a definite metrical-based Chern-Simons singularity.  Yet, since we are here to be initially discussing the actual versus the theoretical -- the actual approach of the so-stated orbifold eigenset that is towards the said Laplacian-based y-based axion, -- will work to bear, in reality, an external angular momentum -- that is to work to bear more of an abelian geometry of approach than a non-abelian geometry of approach, -- since the earlier said assymptotic motion of the said orbifold eigenset towards the so-stated Laplacian-based y-based axion, is to here, only be the physical result of what is simply an approximation of an assymptotic method of behavior.  (Nothing that is actually physical, is likely to just get more and more infinitely closer to any mapped-out axion, without ever to be able to spontaneously cross such a given arbitrary axion, no matter how long such an activity is to happen.  So, in reality, if such an approach is to be prolonged, such an orbifold eigenset will always tend to eventually alter from the theoretical assymptotic behavior, that has here been eluded-to.)  Based upon this just mentioned physical condition -- such a genus of a crossing of a Laplacian-based axion, will, in the "real world," not necessarily work to involve a Lagrangian-based Chern-Simons singularity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Second Part Of Session 4 Of Course 20 -- Calabi Manifolds And Calabi Interactions

There is electrodynamic energy all over the place, throughout the space-time-continuum.  Light of one form or another, tends to be associated, in general, with all mass and kinetic energy -- since even dark matter tends to have a certain amount of heat energy associated with it, -- and heat is a form of electromagnetic energy, that is known of as infrared electromagnetic energy, or infrared light.  There is, as well, electrodynamic energy, that tends to be often associated all mass-bearing orbifolds over time -- in the form of the motion of electrons and other dynamic sub-atomic particles, -- since such sub-atomic particles often have a charge-based characteristic, and the motion of charges works to form the tendency of a multiplicit generally electrodynamic tense of energy.  Almost anything that you tend to see in our visible universe, is most directly associated with the interactions of light with the activity and the existence of electrons, as such electrons, when these are within the Ward-Caucy bounds of atom, work to orbit the external physical bounds of the multiplicit array of atoms.  Whenever light-like phenomenology works, in so as to directly interact with electrons in a Gliosis-based manner, this general genus of interaction -- works to form a general Rayleigh-based scattering, this of which acts, in so as to work to form what may be called a Calabi-Yau interaction.  This is the generally most common form of a Calabi-Yau interaction.  Yet, when any form of a scattering of electromagnetic energy with any form of mass, happens in a Gliosi-based manner, this is actually one form or another of a Calabi-Yau interaction.  Calabi-Yau interactions are the process of that reaction, by which electromagnetic energy is to scatter upon a direct contact with any mass-bearing eigenstates.  Such a Gliosis-based contact, works to form a Rayleigh-based scattering of the said light-like energy -- to where the said energy is to be annharmonic in its displacement right before its re-quantization, -- to where such a re-delineation-based process it to then work to produce both heat and/or other resultant electrodynamic energy -- which is to thereby work to allow for both a freeing-up of the motion of such so-eluded-to mass-bearing orbifolds, as well as then providing for other needed re-organization-based characteristics, upon both the said increments of both mass and light-like energy, that are then needed in so as to work to allow for the flow of the motion of both the correlative mass and the correlative electromagnetic energy.  This general flow of the needed kinematic activity, works to help to keep the relaying of motion active -- for the multiplicit Rarita Structure, -- by the then resultant perpetuation of those vibrational oscillations, that exist along the said multiplicit Rarita Structure eigenstates, -- in the form of the resultant continuation of the flow of those Schwinger-Indices, that act as gravity waves, over the multiplicit sequential series of group-related instantons.  In the process, such a general tense of activity -- works to form entropy.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The First Part Of Session 4 Of Course 20 -- Calabi Manifolds And Calabi Interactions

Light travels in many multiplicit locations.  Light is the most commonly thought of form of electromagnetic energy.  Electromagnetic energy is energy that oscillates via both an electric field and via a magnetic field -- to where the said magnetic field is wrapped-around the said electric field, as is according to the right-hand-rule.  In the process, electromagnetic energy, in general, travels through countless genre of Hamiltonian operands, as such so-eluded-to general beams of electromagnetic energy, is as well to be propagated through the directly corresponding countless Lagrangian-based paths.  The Hamiltonian operands, via which light is to travel through, would here be the correlative space-time-fabric entity-like mediums -- through which such said electromagnetic energy is to travel or propagate into, as such said energy is to here be translated through its correlative delineation-based process, via the sequential series of group-related instantons, in which  light-like energy is to be both delineated and re-delineated.  The directly corresponding Lagrangian-based paths, in which and through which light is to be transferred -- via its correlative Fourier Transforms, would here be the actual mappable-tracings, as to the denoted directorial-based loci, via which the said electromagnetic energy is to be translated from one spot to another.  As such light-like energy is to here be both translated and re-translated, as the propagation-based eigenstates, that are to here be propagated as the multiplicit discrete quanta of such energy, that has both core electric and core magnetic propensities, that are kinematic in the process of their dual torsional Hamiltonian-based operations, -- this quantized said light-like energy is to then exist as the "standard-bearer" of the relationship of all physical phenomenology, via which the relativistic relationship of all physical holonomic substrates may then be associated with each other -- via that component that works to bring the multiplicit arena of physicality, to then exist among themselves.  This component that I have just mentioned is gravity.  Light-Like energy forms the relationship of relativity, while gravity brings physicality amongst other physicality.  The common denominator that exists between light and gravity, is the Rarita Structure.  The Rarita Structure is mainly controlled by the multiplicit oscillations of the correlative light-cone-gauge eigenstates.  Such oscillation-based vibrations, that are to here be on the relative Real Reimmanian Plane -- are to here be subtended into bringing together phenomenology, via both gravitons and gravitinos -- the latter of which, are to here exist off of the correlative Real Reimmanian Plane.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.