Thursday, March 17, 2016

A Little About A Rebounding Orbifold Eigenset

Let us consider here an orbifold eigenset, that is to rebound from off of a relatively superconformally invariant set of orbifold eigensets -- to where this latter mentioned set of orbifold eigensets is to be in a proximal localized state of static equilibrim, that is at the Poincare level to the cite where the said initial orbifold eigenset is to collide with the so-stated Majorana-Weyl-Invariant associated set of orbifold eigensets.  Such a so-eluded-to collision will tend to cause the rebounding orbifold eigenset of such a given arbitrary case, to accelerate into a relatively reversal of its initially so-eluded-to holomorphic direction that it was initially traveling through -- via the relative reversal of its Lagrangian-based path, through a relative reversal of its projection upon its directly corresponding Hamiltonian operand, over the immediately ensuing sequential series of group-related instantons.  Such a so-stated acceleration in the Fourier-based motion of the initially said orbifold eigenset, will tend to accelerate the pulsation of the said respective eigenset -- to where there will consequently be the formation of a set of either Real Reimmanian and/or Njenhuis-based metrical-based Chern-Simons singularities.  This case scenario will tend to be of the Fourier-based activity, that is of the rebounding of one mass-bearing orbifold eigenset that is to interact here upon a more stationary and larger set of mass-bearing orbifold eigensets.  Such a so-eluded-to collision of two different masses, will tend to form a friction that will work to produce heat energy -- that will be transferred, at least in part, upon both of the so-eluded-to sources of mass-bearing holonomic substrate of metrical-gauge-based  Hamiltonian operation.  This will then tend to result in a source that, as well, will then work to form a Calabi-Yau interaction upon both of the so-stated sources of mass-bearing Hamiltonian operators of a metrical-gauge-based physical phenomenology.  Such a spurious formation of metrical pulsation, will then tend to form a spontaneous and eventual ebbing -- that will go into a gradual attenuation of the initial acceleration of pulsation -- due to the condition that physical phenomenology tends to go into the direction of optimum rest.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

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