The Last Part of the Fifteenth Session of Course 17 About the Ricci Scalar

When light -- or any other form of electromagnetic energy -- scatters, the non-kinematic perturbation of the directly appertaining orbifold eigenset of any given arbitrary case, becomes kinematic, since the correlative electric field and the correlative magnetic field of the said discrete increment of electromangetic energy that is being considered here are then not kinematically differentiating in a harmonic manner.  (This is in terms of the entropic condition of the said electromagnetic energy, as it is traversing upon any other medium in a spurious-based manner, over time.)  Light, when scattered, is both non-kinematically and kinematically perturbated, over that directly affiliated duration of group related instanton in which the so-eluded-to electromagnetic energy operates upon the holonomic substrate of any other physical phenomena -- in any manner that may be described of as a Gliossi-based intrusion of the said light upon any other physical phenomena, over the directly associated Hamiltonian operation that I have described in general here.  This means that whenever light scatters upon any physical phenomenon, the light acts as a Hamiltonian operator, that would here act upon the substrate that it scatters upon -- in such a manner in so that the acted upon physical phenomenon will here act as a tense of being a Hamiltonian operand.  Electromagnetic energy acts in a minimum of ten spatial dimensions plus time, since it acts in the manner of being in a p-field.  The nucleus of an atom exists in an f-field -- since it involves a minimum of four spatial dimensions plus time. Most of the mass of any atom comes from its nucleus.  An electron exists in a d-field -- since it involves a minimum of six spatial dimensions plus time.  Most of the electrodynamic energy of an atom comes from its electrons.  Besides certain neutrinos, an electron is considered to basically be a point mass.  So, its of no surprise, that when an electron drops an energy level --in which it temporarily gets closer to its correaltive respective nucleus -- it releases a photon, which is a discrete unit of electromagnetic energy.  This discrete unit of E.M. bears a minimum of the addition of the number of spatial dimensions in an f-field plus the number of spatial dimensions in d-field, or ten.  What I mean by E.M. bearing partially hermitian singularities, is that it bears a smooth Lagrangian-based topological path (in a vacuum), except for the conditions that would here exist at the Poincaire level of the  permutations of those world-sheets, that directly appertain to those changes of directoral-based course of action, that are essential, -- due to the process of the scattering of the so-stated light.  These said world-sheets usually go from having a relatively larger annulus to having a relatively smaller annulus, as these are traceable over the course of the mapping the correlative cohomologies of light, over time.  Any change in the scalar amplitude of the diameter of the annulus of any cohomological-based world-sheet, is a tense of bearing a permutation in the directly appertaining world-sheet-based cohomology.  Any given arbitrary topology is said to be partially hermitian, in this case, when one or two -- generally two -- of the Ward-Caucy conditions of the flow of the directly appertaining cohomological-based indices, are not differentially smooth in the harmonics of their flow -- when this is taken through the mapping of the motion of the correlative substringular holonomic substrate that is being considered here, over time.