Lorentz-Four-Contractions and Oscillations

The Lorentz-Four-Contractions involved with a given arbitrary directly corresponding two-dimensional core-field-density of an affiliated given arbitrary one-dimensional superstring of discrete plain kinetic energy permittivity works to make the so-stated one-dimensional superstring appear as a vibrating ring, when such a superstring is moving within the Ward-Caucy bounds of a directly affiliated electron that is not here in the process of dropping an energy level -- at the Poincaire level that is Gliossi to the outer fringes of the so-eluded-to core-field-density of the said superstring. Over the course of a directly corresponding group metric in which the directly previous conditions of activity are happening to such a given arbitrary electron, those give arbitrary two-dimensional superstrings of discrete energy permittivity of that electron that work to form the discrete increments of its mass will work to bear a three-dimensional core-field-density that would then here appear as a vibrating cylinder, when such a superstring is moving within the Ward-Caucy bounds of the so-stated electron that, again, is not dropping an energy level during the so-eluded-to scenario -- at the Poincaire level that is Gliossi to the outer fringes of the so-eluded-to core-field-density of the said superstring of this second case.  This directly previous scenario will then work to form two and three-dimensional field pockets that will act as orbifolds -- that come together in so as to form that given arbitrary orbifold eigenset that is known of as an electron.  Such an integration of partial core-field-densities, that work to form an overall core-field-density of a common subatomic particle, work to perform those operations that are involved with the Chan-Patton functionablitiy of an electron -- in this given case -- in the course of a sequential series of iterations of group instanton, that works to bear a gauge-metrical basis that may here be considered as a fractal of a covalent operation that behaves as a reverse-fractal of a Hamiltonian nature.  The convergence of the operations of those orbifolds, that are within the so-eluded-to orbifold  eigenset of a non-perturbated electron, that come together in so as to perform a common function as one entity -- is fascilliated by the nature of the quaternionic-instanton-field-impulse-mode. -- The here eluded-to interdependance of the activity of the directly associated homotopic residue, that is involved with the said given arbitrary activity of any non-perturbated electron, is maintained as a topologically sound entity -- via the kinematic activity of the process of Cassimer Invariance.  For example, the superstrings of a non-perturbative electron may, at time, switch Laplacian-based relative neighborhoods -- when in terms of the mappable tracing of those orbifolds that are here inter-laced within the orbifold eigenset of such an electron.  Such a relative local rearrangement of the regions that may be mapped-out from within the Laplacian-based setting of an electron, would then be delineated as a convergent-divergent-convergent sequential series -- in which the directly affiliated wave interactions would bear a conformally invariant condition of hermicity that would have at least some sort of a flush Minkowski topological sway that would be distributed, as the Laplacian-based delineations of such a non-perturbated electron would here involve a local re-allocation of the internal orbifolds that work to comprise the said electron. This, though, does not rule out the condition that the added dimensionality of the electron would still involve tensors that would produce a certain degree of Chern-Simmons singularities that would be driven via both the permittivity and the impedance of such a non-perturbative electron -- whether such an electron is Noether-based or tachyonic-based.  Such a need for Chern-Simmons singularities is actual because of the nature of the angular momentum of the kinetic energy of even a non-perturbative electron.  For instance, the propagation of the directoral indices of the angular momentum of any electron will tend to follow the path operand of the norm-conditions of the initialized encoding of that electron -- per increment of the sequential series of the motion of such an electron -- as taken as a reverse-fractal of a Hamiltonian-based nature.  Such a Hamiltonian-based nature is most directly proscribed by the internal operational nature of the Hamiltonians of those superstrings that internally function as a group in so as to work to form the momentum-like conditions of the affiliated electron.  Such an encodement works to act as the quantifying operator of the eigenbasis of the wave characteristics of the said electron.