Part One of the Tenth Session of Course 18

The nucleus of an atom exists in a set of one or more Calabi-Yau manifolds -- one per each respective nucleon --  that may be described of as a set of one or more respective F-fields.  This just mentioned manifold-based nature here may be described of as a tense of membranous phenomenology -- of which may be considered here as a group of one or more membranes that are made-up of one or more respective orbifold eigensets, that may be thought of as being comprised of what are here termed of as F-branes, or, F-fields, that would here work to comprise a membranous holonomic substrate of the phenomenology that would here work to make-up the specific unique Calabi-Yau-based manifolds -- of which would here, in part, describe the Ward-Neumman dimensional composition of the Laplacian-based differential geometry of the physical make-up of the Majorana-Weyl-based static conditionality of the so-stated nucleons of this here given arbitrary case scenario.  Sub-atomic particles that would here work to involve physical particles, that at a metrical condition of being at relative rest, are intrinsically codeterminable and codifferentiable in a manner that is compliant in a conformally invariant static equilibrium-based tense, in a minimum of four spatial dimensions plus time, over that sequential series of instantons in which the said nucleons -- of which are present in the so-eluded-to nucleus of one unique respective given arbitrary atom, are in the said given eluded-to tense of a general topological sway, that is conformally invariant at a steady-state-based set locus of substringular neighborhood.   This works to bear a relative rest energy, that is relatively non-perturbative in covariant retrospect to the codeterminable activity of the surrounding electrons, of the said directly related atom -- to where the so-stated topological vibrational oscillations of the so-stated F-branes will here then work to form both a covariant and a codifferentiable parity, and a covariant and a codifferentiable chirality -- of both its radial and its spin-orbital orbifold eigenset-based eigenindices, that work to counterbalance the multivarious fluctuations of those individual superstrings, that work to form the said orbifold eigensets that comprise each individual eluded-to nucleus of the so-eluded-to given arbitrary atom, in such a manner in so that the transversel Hamiltonian-based operations of each of the so-stated nucleons will then here remain at a steady-state.  Such a condition of a steady-state set of Calabi-Yau manifolds will then work to bear a tense of conformal invariance of overall Lagrangian-based motion, that will then bear an odd function of delineatory translation -- to where the so-eluded-to nucleons will then not move transverselly in any spontaneous covariant manner, relative to their immediate environment, to where the relative statics of their Majorana-Weyl-Invariant eigenbasis of the said substringular locus will remain stable as such, but may only bear a minimal eigenbasis of either a vibrational and/or an oscillatory-based perturbative cycle, as may be bearing only in either a spin-orbital and/or a radial-based transmittance that is Yakawa to its immediate environment in a directly corresponding manner.
To be continued!  I will continue with the suspense later!  Sam Roach.