Friday, January 22, 2016

About Certain Interior-Based Metrical Singularities

Let us initially presume the existence of an orbifold eigenset, that is comprised of three orbifolds -- that are initially moving through an inter-bound unitary covariant Lagrangian path, over the spatial premises of the directly corresponding Hamiltonian operand  in which the said overall orbifold eigenset is differentiating through -- in a Fourier-based manner, over a relatively transient period of time.  Each of the three said orbifold eigensets acts as a reverse fractal of an orientifold -- to where the theoretical projection of the trajectory of the so-stated overall orbifold eigenset is to meet at the Gliosis-based Ward-Neumman bounds of the core-field-density of another distinct but different orbifold eigenset, that is located at a cross-product-based locus that is in a state of Majorana-Weyl-Invariance.  The Gliosis-based contact, that would then tend to occur -- would then work to form a Rayleigh-based scattering of the two so-eluded-to entities of holonomic substrate -- if adn when the Yukawa-based Ward-Neumman bounds of the two so-eluded-to orbifold eigensets are to make a direct theoretical contact.  Such an attempted contact would not be of a Wilson-based linearity.  The initially stated orbifold eigenset is here initially forming hermitian singularities -- at the interial-based Yukawa Ward-Neumman bounds of the Hamiltonian-based operation of the so-stated orbifold eigenset of three orbifolds, that was here initially stated.  Yet, if the central orbifold of the initially kinematic-based orbifold eigenset, were to be somehow pulled into a tense of working to form a tense of metrical-based Chern-Simons singularities that are to iterate in a back-and-forth manner -- from an attenuated pulsation from its initial rate of vibration to an accelerated pulsation from its initial rate of vibration -- then, this will tend to work at causing the overall initially so-stated orbifold eigenset to form Lagrangian-based Chern-Simons singularities, to where such a Cevita-based perturbation (a perturbation that moves in the direction of an annharmonic physical condition) will then tend to cause the said orbifold eigenset of three orbifolds that is of a kinematic-based nature to veer out of its initially projected trajectory -- to where the initial expectation value as to the initially extrapolated Hamiltonian format of interaction that is of the contact that was to happen between the kinematic-based orbifold eigenset with the relatively conformally invariant orbifold eigenset -- will then be much closer to null.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

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