Part Two of Session Ten of Course 18, the Ricci Scalar and Kaeler Differentiation

Now, let us consider the Ward-Caucy physical boundary conditions of the dimensionality of one given arbitrary electron -- that is, in the process, orbiting the nucleus of one directly corresponding given arbitrary atom.  The so-stated electron is constantly moving along -- accerllerating around the center of the here respective atom, by both moving along the elliptical Hamiltonian-based path of trajectory of its orbital coniaxial, and, by bearing a tense of a spin-based nature, as well, that is, at this latter based premise, at the Poincaire level of the topological surface of the directly corresponding holonomic substrate, that works to form the Ward-Neumman bounds of that orbifold eigenset that works to form the said electron of this given case scenario.  An electron exists in a minimum of six spatial dimensions plus time -- even in any minimal Fourier-based translation of the integrable Hodge-based indices, these of which work to make-up any respective given arbitrary electron. The Fourier-based translation of an electron happens -- through any delineatory eigenbase of group-related metric, in which the so-stated electron is being redistributed as a kinematic relative group attractor eigenset of superstrings, that move both transversally, radially, and spin-orbit-wise, over a sequential series of instantons.  This six spatially dimension-based field is called a D-field.  the genus of the Calabi-Yau manifold that an electron exists in is known of as a D-manifold, or, a D-brane.  The two additional spatial dimensions, that exist with electrons -- that do not intrinsically exist with nucleons, are two added stretched-out spatial dimensions.  The spin-orbital/radial complex of any respective given arbitrary electron -- that is being delineated and redelineated over time -- works to bear an even function of redistribution function, -- the operation of such a function, of which works to bear the so-eluded-to Fourier-based translation of the codeterminable integrated sum of those eigenmembers that work to comprise the said electron, in such a manner in so that the constant re-directoralization-based perturbation of the Hamiltonian-based angular momenta indices are thence pulled along -- in a manner that will here work to make an electron act as the eigenbase of the translation that here exists between discrete mass, discrete electromagnetic energy, and discrete kinetic energy.  I will continue with the suspense later!  To Be Continued!  Sam Roach.