A photon that is propagating in a line that is straight -- when in multiconsideration of the condition of space-time-curvature -- bears both a spin-orbital momentum and an angular momentum that is operational during each succeeding propagation index of the said photon, as it travels in the so-stated straight manner in a vacuum. Any photon and/or beam of photons that is traveling in an unperturbated manner through a vacuum over time moves in a manner that is straight -- when one considers the euclidean Ward-Caucy conditions of a propagated beam of electromagnetic indices that exists here as a quantized set of one or more photons that operate in so as to perform a given arbitrary function -- of the propagatorial delineations that work to allow for electromagnetic energy to behave as it does. As a partial index of a beam of light, in this here given arbitrary scenario,the index acts as a photon that is pulled in a manner that is terrestrially straight over time at an even velocity (this photon, in this case, is transmitted linearly over time), the said photon -- although bearing no Lagrangian-based Chern-Simmons singularities due to the condition of here not being perturbated from its direct path -- by neither scattering, torsioning, nor a relatively circular wave-tug/wave-pull, does bear a partially hermitian tense of delineation. This is due to the condition that the pulse of the individually so-stated photon -- per each static-based considered coniaxial settings of the said photon -- at each smoothly metrical locus to where the pulse of the said photon goes from increasing in the speed of its spin at certain even intervals, at the directly corresponding group instantons, in which both the coniaxial-based spin-orbital momentum and the coniaxial-based angular momentum at the directly corresponding instanton-based intervals, into altering in so as to be decreasing in the speed of its spin at certain even intervals at the directly corresponding group instantons. This is to which both the coniaxial-based spin-orbital momentum and the coniaxial-based angular momentum at the directly corresponding instanton-based intervals forms a spurious condition of cetain respective elongated to decremented pulsations, while then doing a similar spin-orbital operation at an isometrically stable set of intervals -- yet, with the direction of the angular momentum bearing a directoral wave-tug/wave-pull that is then directed in the relatively reverse holomorphic direction of the here continued holomorphic directoral-pull of the so-stated photon. The whole distance as to the even increase to decrease of static Hamiltonian thrust, that then bears the same even increase to decrease of static Hamiltonian thrust, yet, with the alteration of the angular momentum pull of the mentioned photon going from pushing in the direction of the photons permittivity into pushing in the direction of the photons impedance -- is the distance of the wavelength of whatever the wavelength of the given arbitrary photon is. The wavelength of a beam of light is a measurement of the fluctuation of the electric field that is directly associated with a given arbitrary genus of electromagnetic energy. So, if a form of electromagnetic energy was, for instance, 159nm, for one-fourth of this distance -- the photons that work to comprise the eluded to beam, that goes detectibely straight to our observation in a vacuum -- each partial of photonic basis, each of such photons, gradually -- in an even manner -- increase in their Hamiltonian-based thrust over the course of 3*10^8 iterations (yet over a set of group actions that each are comprised of very many group instantons), each of which happen over many actual instantons. This increase in thrust bears no Lagrangian-based topological sway of the photons, and, this, as well, does not alter the so-stated condition of the photons hermicity. Then, for the second quarter of this wavelength, the Hamiltonian-based thrust is gradually and evenly calmed by a factor of 3*10^8 -- in so as to go back to is most relaxed condition of spin-orbital momentum. For the second half of the activity that the here given arbitrary photon works to complete its wavelength, the difference in the pulsation of the photons at the Poincaire level of their kinematic differentiation is only different, due to the direction of the angular momentum being pulled in the direction of the impedance of the photon, instead of the initial directoral-based angular momentum pull being directed in the direction of the permittivity of the just mentioned photon. For this whole wavelength, the so-stated photon is moving, as a whole, in the relatively forward-holomorphic direction. For any other electromagneitc wavelength, such a tendency is similar, but, the distance to complete such a cycle here would alter -- in proportion to the difference in so as to what the other given arbitary wavelength of the electromagnetic energy here is. The increase of Hamiltonian-based thrust in the pulsation of a photon forms infinite Chern-Simmons singularities, while, the decrease of Hamiltonian-based thrust in the pulsation of a photon forms infinitessimal Chern-Simmons singularities. To be Continued.
I will continue with the suspense later! Sincerely, Samuel David Roach.
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