Part Two of Session 12 of Course 18 -- The Ricci Scalar and Kaeler Differentiation

Since substringular phenomena kinematically differentiate per iteration of group-related instanton in either a transversal, a radial, and/or a spin-orbital manner, cohomologies are mappabley traced-out in a manner that involves either a transversal, a radial, and/or a spin-orbital genus of successive progression -- over time.  Orbifolds may move in any given arbitrary transversal-based manner --  in which such a set of superstrings of discrete energy permittivity, that operate in so as to perform one specific function -- are pulled into, in so as to bear a unique genus of Hamiltonian-based wave-tug/wave-pull, in which the directly related substringular phenomena that is comprised of as the said orbifold, is able to bear a condition of optimum rest.  Such a Hamiltonian operator -- in the genus of a substringular orbifold -- is comprised of the resultant Hodge-Index of the trigonometric sum of the correlative superstringular Hamiltonian operators, and the resultant angular trigonometric sum of the correlative superstringular directoral permittivity, that is associated with the overall wave-tug/wave-pull of the said orbifold, as a whole -- over that successive series of group-related instantons, in which the said orbifold is kinematically differentiable -- through the unique discrete Lagrangian, that the so-eluded-to overall Hamiltonian operator is covariant and codeterminable, over the range of its substringular operand, over time.  So, as an orbifold is re-delineated and re-displaced over time, the projection of its trajectory will be moved kinematically through its surrounding space.  The interaction of substringular phenomena, with either the first-ordered point particles -- even if the said substringular phenomena does not directly physically come into contact with other superstrings in the process (Yakawa, yet not Gliossi upon other superstrings) -- will work to form a mappable tracing, of which will work to form a physical memory of the here initially so-mentioned substringular phenomena, by the said first-ordered point particles that are being re-delineated and redistributed --  as is according to both the scalar magnitude of the degree and genus of motion of the Hamiltonian operator upon the said point particles, &, the Hodge-Index of both sum of phenomenology of the said Hamiltonian operator, and its resultant directoral topological sway -- in so as to form a respective given arbitrary cohomological pattern, of which alters in both its respective genus and mode, over the successive progression of the so-stated Hamiltonian operator -- as it is kinematically differentiable, over time.  To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.