Photons And Rham Cohomology

Let us initially consider a given arbitrary photon -- that is moving transversally via a unitary Lagrangian-based path, -- in so as to work to form a Rham cohomology, over an evenly gauged Hamiltonian metric.  Such a photon may be said to be basically just generating cohomology in such a case (as opposed to degenerating cohomology).  Next, let us say that the said photon is to, all of the sudden, be scattered upon a phenomenology of holonomic substrate -- that such a photon is to eminently become Yukawa towards, in a Gliosis-related manner, -- at an instance of time.  Once the said photon has been scattered -- the consequently entropic photon is to then to briefly be just degenerating cohomology, as it is in the consequent operation of its perturbated Fourier Transform (as opposed to generating cohomology).  As such a so-stated photon is here to have then to have acted as an entropic eigenstate that is, over one relatively transient gauged-metric, to have gone from its prior condition of just generating cohomology -- into a state of Ward-Cauchy-based conditions, to where it is instead to be just degenerating cohomology, -- the photon of such a given arbitrary case scenario, that has just become entropic, is to now be moving along in such a manner -- to where it is to then to be working to form a Doubolt cohomology, -- in so long as the so-stated photon is in the process of scurrying via  the process of radiative scattering.  Once the said photon is to go back into quantizing with other light, -- then, the said photon will tend to return to going back into the tendency of basically  just  generating cohomology, via the Hamiltonian processes of a consequently formed Rham cohomology -- that will be aptly utilized instead, in such a case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Yukawa Kahler-Metric

The more Yukawa that the Kahler-Metric is, to any one given arbitrary discrete quantum of energy that is at one set gauged-metric, -- the more asymmetric that the adjacent gauge-bosons of the said respective given arbitrary discrete quantum of energy will then tend to be.  The more asymmetric that the adjacent gauge-bosons of any one respective given arbitrary discrete quantum of energy will be, -- the more harmonic that the resultant formed Schwinger-Indices that act as gravity waves, will then tend to be.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.