Part Two as to Displacement Magnitudes

Once that the relative so-eluded-to Dirac is completed by the convergence of the series of wave-iteration -- that is shared at a relative distance, that, because of the same relative covariant differentiation of roll, spin, and first-ordered-point-particle-based-reformation -- act here in a proximal-based manner -- the directly associated strings will here work to exist in state of static equilibrium, when such superstrings of discrete energy permittivity are here considered as here being relative to one another, to where a fractal of an internal magnetic shift will then here work to maintain its magnitude -- by not "hyper-extending" in terms of its correlative core-field-density.  (The directly associated mini-stringular-based segments will bear at least some degree of a genus of a non-abelian-based differential geometric spatial association, for the directly associated eigenbase of holonomic substrate, to where, this is to tend to happen over the directly corresponding sequential series of instantons, in this given arbitrary case.)  Since the homotopic Ward-Caucy conditions that I have just worked to describe here, for the 10 million initially considered supertrings, will interact as proximal in the substringular-based scenario, this Hamiltonian-based orbifold eigenset that I have here eluded-to will act as if these states of discrete energy are relatively adjacent, at the vantage-point of an observer that may extrapolate a detection of such eigenstate-based indices.  Such homotopies that exist, per superstring, tend to exist outside of the stringular band level -- to where those holonomic substrate-based indices that are here most affected by the exterial-based photons that I had mentioned as part of the scenario that I had implied in my last post, will be less affected by the so-eluded-to fractal of magnetic field. (The spin-orbital momenta of superstrings that have just been scattered by photons -- will tend to bear a higher genus of interaction with a conformal invariance that is associated with their angular momentum, than with the conformal invariance that is associated with its roll, over a relatively transient duration right after the so-eluded-to scattering.)  This is, while those superstrings that are more codifferentiable with the band level of the here overall resultant field homotopy, by not bearing as much of a Gliossi-based interaction with the so-eluded-to photons -- will tend to bear more of a fractal of magnetic conformal invariance, since the here correlative spin-orbital permittivity of this set of superstrings will be able to bear a relatively more invariant mode, when in terms of the static equilibrium of its relative roll. So, a homotopy that has an analogous spin, roll, and pointal reformation, per general iteration of group instanton -- will tend to behave to where the just implied orbifold eigenset will bear a higher potential as appearing as a whole group, that will act as adjacent, to where  that general condition may be detectable as acting as one proximal set of substringular indices -- which will work to form a more potential fractal of magnetic-based attraction.  Session 6 next.  Sam Roach.