Course 20, Session 10 -- Part One

Light and all other forms of electromagnetic energy, tend to travel in multiple beams of energy, that are interconnected -- via a process known of as quantization.  Any electromagnetic energy that is here to be propagated, is to be transferred through space and time, in discrete bundles of photons, -- of which are here to be delineated upon their environment, in the form of one or more beams of energy, over the course of the general duration of time (and in the path of least time).  Different types of electromagnetic energy exist in different beam-related bundle sizes, of which work to help in causing the general condition of the many different sizes of wavelengths of electromagnetic energy -- that are here to exist as differentiating in a kinematic-related manner, over the multiplicit sequential series of group-related instantons, that are to be happening in realm of the light energy and the light matter that exist in physical space and time.  Such so-eluded-to variations in the genre of the different sizes and types of wavelengths of electromagnetic energy that are to exist in the multiverse, helps to form the individually taken operations that each specific genus of electromagnetic energy is to form -- as such electromagnetic energy is to work to influence its environment in an interdependent manner, as such said energy is to be Yukawa to other energy in the realm of space and time.  All motion exists relative to both the existence and the velocity of light, over time. Photons exist in p-fields, and photons, when individually taken, are the discrete increments of electromagnetic energy.  All light and all other forms of electromagnetic energy, exist in integer-related packets of one or more photons.  Therefore, this happens in such a manner, to where all motion exists relative to both the existence and the velocity of the general genus of the most important generic type of p-field, -- to where all motion exists relative to light.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Info As To Adjacent Electrons

Electrons exist in d-fields -- of which exist in a Fourier-based manner, in at least 6 spatial dimensions plus time.  Photons exist in p-fields -- of which exist in a Fourier-based manner, in at least 10 spatial dimensions plus time.  Any hermitian-based flow of the spinning motion of a particle that would here exist in a Fourier-based manner in 6 spatial dimensions plus time, will tend to often bear a change in the sixth derivative as to the Ward-Derichlet conditions of the perturbative tense of the overall directoral-based discrete momentum, that is of that said given arbitrary respective particle.  This means that any given arbitrary electron, that is differentiating as a Hamiltonian operator in a Fourier-based manner, in such a way in so as to be of a Yau-Exact manner -- which would then be as a hermitian particle -- this will then tend to bear an overall directoral-based discrete momentum, that will then often tend to change in the sixth derivative as to the Ward-Derichlet conditions of the perturbative tense that is of that so-stated electron, over time.  When an electron undergoes the Fujikawa Coupling, which happens via the Green Function -- which is as is according to Chan-Patton rules -- it will then form a photon, and, a photon exists in a p-field -- this of which exists in a Fourier-based manner of which exists here in at least 10 spatial dimensions plus time.  Let's say that an electron is differentiating in a Fourier-based manner -- by such a means that would here work to involve, in this case, a condition of only two genre of dimensional-based tensors -- in such a manner to where a discrete increment of the kinetic energy of that so-stated given arbitrary electron, would then exist in eight spatial dimensions plus time -- immediately before it is to go through the respective said eigenmetric of the said Fujikawa Coupling, -- then, as the so-stated discrete increment of kinetic energy that is being released from the said electron, is going through the so-stated process of the respective eigenmetric of the Fujikawa Coupling, which is at that inferred general locus in the substringular in which the so-eluded-to discrete increment of quantum energy is here being converted into a photon -- there will then tend to be a binary Lagrangian-based Chern-Simons singularity, that would then be formed in the process of the said eigenmetric of the here proximal localized activity in which the Fujikawa is to here be happening at.  This process works to cause any given arbitrary respective photon -- that is formed by the process of any given arbitrary respective electron that has here just dropped an energy level -- to tend to be pulled-out of the Ward-Neumman bounds of the respective atom in which such a discrete increment of the kinetic energy of an electron is converted into a discrete quantum of electromagnetic energy.  This is indirectly why there is the Chan-Patton-based condition, that electrons that are adjacent must always bear an assymetric spin -- in order for such electrons to not totally impede upon each others space.  This latter point is the Pauli-Exclusion Principle.  I will continue with the suspense later!
Sincerely, Samuel David Roach.

More About Orbifolds & Gauge Fields

An orbifold exists as a set of superstrings that exist as an organized unit with a first-ordered magnetic eigenstate associated with it. The spin-orbital field delineation of the superstrings of an orbifold act as second-ordered magnetic eigenstates of the substringular condition. The orbifolds of an orbifold eigenstate integrate through first-ordered magnetic eigenstates to form the magnetism of an orbifold eigenstate. This magnetism bears a gauge-field that induces an electrodynamic group gauge-action of Majorana-Weyl covariance between D-fields and F-fields in the environment of P-fields. The shell-like structure of an orbifold bears a periphery of substringular fields and gauge-fields that bear a norm Ward relationship in terms of the unborne tangency of Fadeev Popov Traces, along with the Yakawa and Heisendorf cohomological and nonabelian interactions that allow the superstrings of the correlative Fadeev Popov Traces to bear a tense of group harmonics, which via gravitational interaction included, draws among and upon the associated superstrings a set of Klein-Kaeler-Higgs impulses that allow the substringular forces to bear an interactive relationship with each other that is global yet discrete. The interior of the interactive stratum shell of an orbifold often has an interactive shell that is Chern-Simmons bound to the stratum of one parallel universe eigenbasis as another stratum of parallel universe. This causes all mass index shells to have a core density that integrates all of the interior of such a potential shell when there are interactive parallel universes in an orbifold. The Fadeev Popov Traces, as said before, are norm relative to one another if these are of the same universe with a wobble of ~1.104735878*10^(-81)i degrees. The more remote a universe is relative to a given universe, the more off the unborne tangency of the respective Fadeev Popov Traces are in terms of the cross-sectional geometric Laplacian taken at BRST. The gauge-fields of these discrete substringular Planck related phenomena of different universes relative to one another in certain orbifolds are interbound with a tendency to bear some field cohomology. The differing norm conditions of these associated gauge-fields causes the correlative second-ordered light-cone-gauge eigenstates to remain abelianly for Kaluza-Klein topology and non-abelianly for Yang-Mills topology unscaffed yet interactive via the Yakawa-bound norm state fields that, are commutative via the Cassimer Invariance that indistinguishably differently recycle the norm states to ground states, and the ground states to norm states, after a successive set of iterations that are based on a Fourier sequential series that transforms the substringular and gauge-fields one eigenlocus at a time into a fresh substringular and light-cone-gauge eigenstate field. The case of an orbifold region that is completely of one univerese will be Laplacianly conditioned as a majorized stratum that bears an internal charge density, and is of a Hilbert structure that bears multiplicit eigenstates of Minkowski based Majorana-Weyl magnetic eigenstates.