As To The Attraction of an Electron To A Proton

As everyone knows, any given arbitrary  electron of a respective atom -- which is considered to have a negative charge -- is physically attracted to a proton -- which has a positive charge.  An electron has an attraction-like tendency to be have a momentum that is drawn inward (as is like a relative cross-product-based wave-tug/wave-pull (into the page)) , in so as to have a bearing, that, if it were not traveling at close to the speed of light -- it would be pulled inward into the region of the directly corresponding atom, where there are the protons or the proton, that is at the nucleus of the correlative atom.  Any given arbitrary proton, which is considered to have a positive charge, as everyone knows,  bears a tendency of a wave-tug/wave-pull -- that is physically attracted to a directly corresponding electron of the correlative atom.  From the relative vantage-point of any respective given arbitrary proton, the pull of the attraction of the respective given arbitrary electron of the correlative atom -- in which the said proton exists in, happens in such a manner, in so that the proton has a tendency of having a magnetism that works at attempting to pull the correlative respective electron inward, toward the so-stated proton -- in a dot-product manner ("out of the page").  At the substringular level, whenever there is a genus of the perturbation of the superstrings of any one set of the respective orbifolds -- that work to comprise part of such a stated given arbitrary atom -- in terms of the directoral-based conditions  of the correlative Majorana-Weyl-Invariance, that is of the proximal general locus of such a case,  as to the directly correlative Ward-Caucy boundary conditions -- to where this genus of the perturbation of the so-eluded-to superstrings of discrete energy permittivity, works to reverse the here relatively holomorphic direction of the topological sway of the said respective given arbitrary superstrings of such a given case, then, one will tend to have a bearing of what may be termed of as an antiholomorphic Kahler condition.  Whenever this so-mentioned condition happens to a set of superstrings that work to comprise an orbifold eigenset -- this causes what is known of as a Wick Action to happen.  This works to form the activity of an ensuing Kahler-Metric eigenstate -- in so as to help with both the persistence and the continued existence of the local discrete energy of a specific given arbitrary region of superstrings.  So, if the directoral-based topological sway of the Majorana-Weyl-Invariant eigenbase of any respective given set of superstrings -- that are of any given arbitrary atom, is altered into a reversal of its Lagrangian-based flow, over a relatively transient period of time in the substringular -- this will work to form what would be here a proximal group metrical activity of the Kahler-Metric.  Such a tendency of the Kahler-Metric happening, as such, works -- at the atomic level -- to help to conserve energy, when the alteration of the respective activity of an atom would Otherwise work to attempt to reverse the charges of the sub-atomic constituents of any respective given arbitrary atom.  This way, there is a conservation of charge to be more viable.  To Be Continued!  Sam Roach.