Solution To The Second Question Of The Last Test Of Course 11

When one takes orbifold indices of adjacent Planck-like phenomena, the corelative orbifold indices bear the same relativistic wobbling as their corresponding agular momentum eigenstates -- an angle of wobble that is corariant, codifferentiable, and codeterminable by ~1.104735878*10^(-81)I degrees. Again, the bearing of norm-state-based relation depends on the relativistic layer of adjacency that one Planck-like phenomenon exists at relative to another PLP (Planck-like phenomenon) from the same universe -- as may be extrapolated via the right-hand-rule.  This is here in a relationship that exists between one PLP from one orbifold that is of the same universe as another given arbitrary PLP from another given arbitrary orbifold.  (The reason as to the term "Planck-like phenomenon" or Planck-like-phenomena is that ideal adjacent discrete units of energy impedance -- Planck-like phenomenon when taken individually or Planck-like phenomena when taken multiplicitly -- are only existent as one out of every trillion of such discrete units of the said energy impedance.)  The stated indices are ideally the multiplicit-based index relationships of one PLP of one orbifold of one given arbitrary universe to one or more other PLP of one or more orbifolds that exist in the same given arbitrary universe.  Ninety degrees means pi divided by two.  Two tmes 32 is 64.  Thus, the norm-state solution that brings one back to a 90 degree physical mapping out Laplcian-based relation is when one goes out 64 layers  of adjaceny out from an initial layer of adjacncy.  The levels of adjacency mentioned here are not specifically bearing on the conditions of relative proximity. I will continue with the solution to question three of the said last test later!  Sincerely, Samuel David Roach.