As To The General Basis For Magnetism

In terms of the substringular -- magnetism is that condition that tends to happen when one set of superstringular phenomenology, that bears a relatively knotted constitution of construction, works at bearing such a wave-tug/wave-pull -- in so as to either push-out and/or bring-in other tenses and/or genre of a superstringular phenomenology that here bear either the same or a relatively less knotted constitution of construction.  So, when such a general tense of a magnetic pull is happening among masses that work to bear an electrostatic wave-tug/wave-pull upon each other -- magnetism tends to happen when one orbifold eigenset, that works to bear one respective given arbitrary genre of centralized knotting, works at bearing such a wave-tug/wave-pull in so as to either push-out and/or bring-in other tenses and/or genre of a superstringular phenomenology that bears another respective given arbitrary genre of centralized knotting.  So, when one is to have an orbifold eigenset -- that had initially been in the process of being magnetically pulled or pushed in a state of static equilibrium by another orbifold eigenset,  over  the course of what would here be an occurrence that is happening in a tense of conformal invariance -- to where then, all of the sudden, the general direction of the so-eluded-to magnetic thrust is then reversed, in such a manner to where the directorial-based integration of the so-eluded-to Lagrangian-based path, that the here initially so-stated orbifold eigenset is to then reverse in its holomorphicity -- to where, this genus of activity will then tend to form an antiholomorphic Kahler condition.  This will then lead-up to the formation of the activity of a Kahler-Metric.  As such a so-stated perturbation of the general magnetic field is to happen here to the two so-eluded-to covariant orbifold eigensets, the Ward-Caucy boundaries and the two respective Majorana-Weyl-Invariant-based modes will just as well alter -- one of such Majorana-Weyl-Invariant-based modes for the first of such mentioned given arbitrary orbifold eigensets, and, another of such Majorana-Weyl-Invariant-based modes for the second of such mentioned given arbitrary orbifold eigensets.  This will then work to re-delineate the loci of the proximal-based cites of the two inherent respective genre of that centralized knotting -- that will here be of that general condition of holonomic substrate, that will have here worked to glue or stick those subatomic particles together in so as to make the constitution or make-up of the two individually stated orbifold eigensets that I have been discussing here in this given arbitrary case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.