Electromagnetic energy, including all light, tends to scatter at least to some extent -- if that electromagnetic energy is propagated in an orthogonal nature, upon any given surface of any phenomenon, that the given electromagnetic energy is interfacing upon. Whenever any electromagnetic energy is orthogonally transferring and propagating through and/or upon a surface or region, the given electromagnetic energy is then to tend to be polarized at least in part, through and/or upon the given surface or region. However, when electromagnetic energy, in the form of quantized beams of waves, is orthogonal as a field -- to any plain kinetic energy that exists as a field, then, the said electromagnetic energy will tend to be absorbed as opposed to being scattered. If the given electromagnetic energy is not completely polarized, and is thus scattered to some degree, then the electromagnetic energy that is here to be striking a tense of plain kinetic energy in a manner by which it is scattered, must then switch its genus of topology, right after the light is to scatter upon the surface of the given said plain energy. That would mean, that the electromagnetic energy that is scattered here, would change temporarily, from initially having a Yang-Mills topology to then working to bear a Kaluza-Klein topology. This here would mean that the Clifford Algebra here, would then be converting from working to bear a euclidean and hermitian geometry, into then working to bear a euler and Dirac geometry, for the time being. Once that the given electromagnetic energy is scattered, the Gaussian of the superstringular part of the said electromagnetic energy, is to switch back in its light-cone-gauge orientation.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
No comments:
Post a Comment