Solution 8 Of Test 2 Of Course 20

From the time that any one given arbitrary photon is to be scattered, until it is re-quantized back into a beam of light -- such a so-eluded-to entropic photon, is here to toggle from being delineated at a Laplacian-based extrapolation, in an orthogonal manner from its initial directoral-related tense of holomorphicity, -- as one may trace such a delineation from the point of scattering up to the covariant positioning at which it is to ensue in so as to re-quantize back into a beam of light, to then toggle back into being delineated at a Laplacian-based extrapolation, that is here to then be able to be extrapolated as working to bear a tense of holomorphicity, --  that is in a general linear distribution from where the photon was to have been scattered, up to the covariant positioning at which it is to re-quantize as I have mentioned earlier, back to toggling back into the earlier mentioned general genus of orthogonation ( a tense of Ward-Polarization, that may be traced in an extrapolation from its space-related point of scattering up to where its is to be re-quantized), and so-on, -- until the here initially stated entropic photon, is to be brought back into the beam of light as a Yang-Mills-related topological phenomenon that is here to bear partially Yau-Exact singularities. (To where the said photon is to go back into being as a standard discrete quantum of electromagnetic energy over time.)
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

The 9th Session Of Course 20 -- Part One

Light always travels in a given framework of topology.  The framework of topology that light travels in when the given light is approaching a phenomenon that it is about to scatter upon, is different from the framework of topology that it travels in -- at the moment right after the light has scattered upon a phenomenon, -- the last of which is different from the framework of topology that light travels in when the given light is to go back to being quantized with other light.  This just stated general condition is true not only about light -- yet it is as well as true with any other genus of electromagnetic energy.  The topology involved with any actual beam of electromagnetic energy, has a different framework than when the given electromagnetic energy is scattered.  The same set of eigenindices that had initially worked to comprise the here stated electromagnetic beam just as it is being scattered, has a different topological framework from the light-cone-gauge topology of the just eluded-to Ward-Cauchy-based condition, once that said energy is requantized. Actual light, as well as all actual electromagnetic energy besides light, travels with a Yang-Mills light-cone-gauge topology.  This means that all of the light-cone-gauge eigenstates that work to comprise the primarily wave-based discrete energy impedance-related quanta, that are here to work to comprse this so-stated electromagnetic beam -- are of a non-abelian nature.  This means that all of the second-ordered light-cone-gauge eigenstates that are here to work to comprise each of the correlative individually taken first-orderd light-cone-gauge eigenstates, that are of each of the directly corresponding discrete energy quanta, that are to come together in so as to work to form the said beam of light, are to exist as Laplacian-based sinusoidal waves of "twined" mini-stringular segmentation -- that are to be fed-in to the proximal locus.
I will complete the idea that I have just started here soon.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Session 10 of Course 14

Photons go away from the locus of those electrons that form these -- once that the corresponding electrons drop an energy level in so as to form the said photons.  When photons form, these are brought to into the direct vicinity of other photons in such a manner is so that these work to coallece into one one or more beams of light -- depending on whether one is here considering one or more groups of photons that respectively quantize into one or more beams of the eluded to electromagnetic energy.  One of the main properties that causes photons to coallece is the condition of the whole-spin of the individual photons that work to quantize -- in a discrete manner -- into beams of electromagnetic energy, primordially, light.  The angular momentum, spin-orbital momentum, and, the specific parity of any set of respective photons -- relative to one another -- works to bring certain relatively local photons together with each other in so as to allow these said photons to coallece into a beam.  The just mentioned coalleceing, or, the eluded to quantization that I have just described, works to make each photon that comrpises any corelative beam that such phenomena come together to form, to act as both an individual photon, &, also as the whole beam of the corresponding electromagnetic energy, at the same time.  The said quantization of light brings light together into beams of light -- while, in other arbitrary cases, this said general condition of quantization, often, in many cases, works to bring certain beams of light into a larger scope of electromagnetic energy that would here work to form a wider "arena" of the relatively proximal electrodynamics that exists in a given arbitrary general region of kinematic-based space-time-fabric.  Photons travel in a straight line in a vacumm. -- In so far as space-time may be considered as relatively "straight" in a limited distance in which such a detectable extrapolation may be determined.  I put it that way, on account of the condition that space-time-fabric actually tends to curve over a much larger extrapolation-based distance.  The electric fields of beams of photons do not fluctuate in a straight line.  The just mentioned fluctuation of the said electric field of a beam of light is the wavelength of that said beam of light.  White light fluctuates to less of a degree in its electric field than infrared electromagnetic energy.  A strong laser fluctuates to less of a degree in its electric field than the said white light.  Photons that have complementary spin, angular momentum, spin-orbital momentum, and directoral parity, will tend to coallece with each other to form a specific form of electromagnetic energy.  When photons with a different spin, angular momentum, spin-orbital momentum, and/or directoral parity, are directed toward each other, theses will scatter until these reach a basis of complementary flow -- once the directly corresponding photons scatter into a genus of a relatively common spin, angular momentum, spin-orbital momentum, and directoral parity -- in so as to quantize as an overall beam.  Sam.