Cohesive Orbifold Eigensets

Let us consider three different sets of orbifold eigensets -- one of which is a set of neutrons, of which bears no charge;  another, of which is a set of protons, which bears  positive charges; and, another, of which is a set of electrons, which bears  negative charges.  Each of such individually taken so-eluded-to orbifold eigensets of which has, what one may term of as one discrete charge.  Let us now say that all three of these orbifold eigensets exist in the Ward-Caucy bounds of one respective given arbitrary atom.  Let us now consider the said atom to be charge-wise stable, over time.  This would then mean that there will here be just as many protons in the so-stated atom of this respective case, as the number of electrons of the said respective atom in question.  The number of neutrons that would exist in the atom of this given case, will here be of an arbitrary amount.  This would mean that the net positive charges that would here be delineated outward from the relative nucleus of the so-stated atom, will be valance-wise countered by the net negative charges that would here be delineated inward from the relative exterior-based shells -- in which the directly corresponding electrons would be existing at.  All of this activity would be happening over a discrete course of manageable time -- even though one could here theoretically be able to map-out the cohomological tracings of the kinematic activity, that is of the interdependent motion of the so-stated positive charges -- that would here be delineated by the orbifold eigensets, that would here be characterized by the kinematic activity of protons, towards the kinematic motion of the directly corresponding charges that would be extended from the orbifold eigensets that would here be characterized by the existence of electrons, these said electrons of which will tend to work to nullify the physical condition of what would otherwise be an existent valance charge, by extending their relatively negative charges inward toward the protons that will here be existent at the nucleus of the said atom.  So, although any atom will always tend to delineate the existence of the various charges, that will here work to comprise these so-eluded-to physical entities -- then, when an atom is charge-wise stable, its overall valence potential will always tend to strike a balance, that is actually a counterbalance that would here be interactive between  the intrinsic positive charges of the correlative atom with the intrinsic negative charges of the correlative atom -- at its proximal atomic-based core-field-density.  And, any physical charges that are delineated -- will be propagated by the kinematic activity of the respective given arbitrary orbifold eigensets, of which will here tend to act in a Fourier-based manner, in so as to work at the existence of what may be termed here as the conservation of charge.  I will continue with the suspense later!  Sincerely, Sam.