Holomorphic-Driven Collinear Homeomorphic Waves

 When two different and distinct covariant holomorphic-driven collinear homeomorphic waves, are to strike "head-on," these two different respective individually taken waves, will consequently tend to result, in working to bear the formation of the general proximal local presence, of a set of anti-holomorphic Kahler conditions, in the general process of working to bear the general condition, of a Ward-Supplemental tense of behavior. This will, in the process, often tend to occur, over the general processes, in which there is here to be the proximal local behavioral presence, of a tense of one or more Chern-Simons singularities, of which are here to be incurred, upon the kinematic gauge-metric-related action, of these two earlier stated different and distinct respective individually taken waves, as such a dual covariant tense of a topological collision, as taken over the Fourier Transform of a respective dual tense of a Lagrangian, is thence to work to bear the general supplemental Hamiltonian inter-reaction, that is of such an inferred Yukawa Coupling, as this is here to be taken, in a spontaneous manner, that is to immediately ensue the inferred Gliosis-Based contact, in which the immediately externalized fields, that are of both of such individually taken Ward-Cauchy-Related waves, are here to work to bear an eminent strike of dimensional-related pulsation upon one another, in so as to work to form the earlier implied condition, of the earlier stated tense of Ward-Supplemental behavior. I WILL CONTINUE WITH THE SUSPENSE LATER!  TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

“Ablated” Homotopic Residue — My Perception

 If one were to take the inversion of the process, of the general gauged-action, of a Noether-based unitary homeomorphic escalating Lagrangian of a Euclidean expansion, one would then tend to have, instead, the process, of the general gauged-action, of a Noether-based unitary homeomorphic attritional Lagrangian, that is of a Euclidean contraction, to where, instead of such a said Lagrangian working to bear a compounded tense of homotopic residue, such an attritional Lagrangian, would consequently tend to work to bear an “ablated” tense of homotopic residue. I will continue with the suspense later! Sincerely, SAMUEL DAVID ROACH. 

More As To Heat And Sound

 The dissonant application of heat, may often be used, in the process of tending to work to accelerate the general processes, of the correlative local bearings of entropy. Whereas; the practical application of resonant sound, may often be used, in the process of tending to work to decelerate the general processes, of the correlative local bearings of entropy. To Be Continued! Sincerely, Samuel David Roach.

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.