Friday, January 11, 2013

Session Four Of Course Eleven About Orbifolds

Planck-like phenomena differentiate relative to each other per iteratioin of group instanton.  The angular momentum indices of the just mentioned Planck-related phenomena get near each otehr while these differentiate relative to one another.  The spin-orbital indices of a Planck-like phenomenon work to comprise its fractal of magnetic field.  The magnetic field fractal of a Planck-like phenomenon surrounds the angular momentum indices of the initially mentioned given arbitrary Planck-like phenomenon.  The angular momentum indices of a Planck-like phenomenon is its fractal of an electric field.  So, the magnetic field fractal of a Planck-like phenomenon surrounds the fractal of its electric field.  The angular momentum indices of a given arbitrary Planck-like phenomenon are relatively near the angular momentum indices of the surrounding Planck-like phenomena.  The adjacency of Planck-like phenomena angular momentum indices that are directly associated in a substringular-based neighborhood works to cause the mentioned fractal of magnetic field -- at a substringular level -- of the relatively associated Planck-like phenomena that are of parallel universes to overlap to a certain extent.  This includes the occasional Yakawa cohomologies and the other Gliossi-based interactions that work to occasionally directly associate substringular phenomena that are of different universes, although, in a manner that is not detectable by any ordinary viable manner.  The angular momentum indices of adjacent Planck-like phenomena that are of the same universe are bear norm-conditions that bear a direct orphoganal-basis with a codeterminable relativistic codifferentiable wobble of ~1.104735878*10^(-81)I degrees -- given the relative wobble of one of such said given arbitrary Planck-like phenomena toward the other and vice versa.  The Planck-like phenomena that are of other universes relative to one another do not share such conditions of an orphoganal-basis with the just mentioned format of wobble, when one considers two different of such Planck-like phenomena that are physically adjacent over a Laplacian that is set at one given arbitrary iteration of group instanton.  This lack of norm-based conditions between adjacent Planck-like phenomena that are of different universes is what works to cause such phenomena to interact as different phenomena that are of different universes.  Yet, the fractal of the magnetic field of different Planck-like phenomena tend to overlap.  This brings up the condition that the orbifold indices of different Planck-like phenomena of different universes tend to overlap.  This means that the fields that are generated by the various orbifolds that are existent in any general given arbitrary locus -- whether these orbifolds are of the same universe or not -- tend to bear some overlapping propensities.  This is due to the Clifford-based expansion of the Ward multipole conditions that are associated with the fractal of the magnetic fields of the orbifolds that exist in the substringular.  This means that the orbifold eigenbases and the orbifolds that inter-relate to the various layers of reality tend to bear a certain degree of Yakawa interaction, or, in other words, these bear a certain degree of overlapping.  This means that the intrinsic fractal of the magnetic fields that exist in the overall interplay that happens in each set of universes is wrapped up to an extent both among all of the layers of reality and also among all of the universes that exist in each set of such parallel universes.  (Every universe is parallel to another.)
I will continue with the suspense later!  Sincerely, Sam Roach.

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