As I have said before, a Campbell norm-state Projection is a holonomic substrate-based trajectory of substringular-based phenomenology, that consists of one respective given arbitrary first-ordered point particle that is connected to a round "plate" or disc of a composite of one or more layers of first-ordered point particles, that are interconnected by mini-stringular segmentation -- in a homotopic manner. The respective given arbitrary said "plate" or disc of a composite of one or more layers of first-ordered point particles of any given unique case, that I have eluded-to here, tends to lead the so-stated Campbell norm-state Projection in the relative forward-holomorphic direction -- in the course of the kinematic translation of such a so-stated norm-state-projection, from one covariant-based locus to the next of such, over time. Otherwise, the said general genus of such a projection would spontaneously collapse -- due to the condition that the "plate-like" phenomenology that works to help comprise the said genus of projection bears a significantly higher Hodge-Index of potential Hamiltonian-based operators, in the form of such a partial of the construction as bearing a significantly higher number of first-ordered point particles at the here inferred general Laplacian-based locus of the said genus of projection. Furthermore, I have mentioned that what may be termed of as a Hausendorf Projection is comprised of two half-shell-like constructions of composites of first-ordered point particles that are distanced and interconnected by mini-stringular segmentation -- the so-stated individually taken half-shell-like constructions here being of a covariant basis of being of a relatively opposite nature of correlative concavity, via the vantage-point of extrapolating along the so-stated Hausendorf-norm-state-Projection in the relative holomorphic direction. Now, if one were to have a circumstance to where one given arbitrary Campbell Projection were to bear a Gliossi-based pull upon one given arbitrary Hausendorf Projection in the relative holomorphic direction, to where the said Hausendorf Projection were to apply a Gliossi-based push upon either a superstring or a cohomological-based index, over time -- over one respective given arbitrary covariant-based group metric -- the interconnection between the plate-like end of the so-stated Campbell Projection would tend to bear a locus of holonomic substrate, where in which the so-eluded-to activity of the eluded-to binary norm-state-projection-based Hamiltonian operation, that would here involve a topological sway, would work to cause the said Hausendorf Projection to either sway, at its forward-holomorphicic end where it is then interacting in a Yakawa-based manner upon the said superstring or world-sheet, either in the relative reverse-norm-to-holomorphic direction (relative downward), or, in the relative forward-norm-to-holomorphic direction (relative upward). This is because, for all intensive purposes, any given arbitrary norm-state-projection will not bear linearity that is of a Wilson-based linearity. A plate or disc-like Gliossi-based contact will tend to bear relatively little slippage, yet, a perimeter of a half-shell-like Gliossi-based contact will tend to bear relatively more slippage. So, if the push that is here made upon the said respective given arbitrary Hausendorf Projection of this case is at all topologically slanted upward, then, this will work to tend to pull the relatively holomorphic end of the said Hausendorf Projection downward, while, if, instead, the push that is made here upon the said respective given arbitrary Hausendorf Projectiion of this case is at all topologically slanted downward, then, this will tend to work to pull the relatively holomorphic end of the said Hausendorf Projection upward.
To Be Continued! I will continue with the suspense later! Sam Roach.
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