Part Two Of The Preface To Course Ten

As to the Yang-Mills light-cone-gauge topology that I previously was just mentioning on the post that I wrote yesterday, if the Yang-Mills supersymmetry is not attained here, then, the holomorphic residue that I was relating in the discussion yesterday will flow after each reiteration between the homotopic indices of the traits that are here physically represented individually as a group of superstrings associated with certain arbitrary norm-projections that each bear a specific eigenfunction.  This genus of the prior mentioned flow causes what I metaphorically denoted as a "fluid" to flow in a manner that forms an alteration of norm conditions and thus an alteration of Gaussian conditions.  If the pseud-magnetic (meaning here a fractal of voltage) coupling involved here increases in magnitude, along with an increase in the related angular momentum (the angular momentum here being a fractal of charge), then, the "fluid" will snap and recoil.  If the holomorphic index is increased in this scenario -- in terms of action intensity during the corresponding Fourier Transformation in which the related superstrings bear a relatively simultaneous covariance when determined at the conicenter of the metrics that are undergoing a kinematic codifferentiation -- then the described kinematics of the directly related eigenstates of superstrings and their affiliated norm-projections will cause the mentioned recoiled sections of "amorphous" quantiative Hodge-Based topological "substance" to begin to "slip" as a folded manifold that here may be either trivially or non-trivially isomorphic.  This would then happen after the proper sequence of iterations and the proper series of wave discharge is initiated so as to allow the prior mentioned coditions to take place.  The said folding of a substringular manifold causes the related superstrings of both of the mentioned traits taken individually to reattain a covariant kinematic differentiation that bears a direct correspondence between both of the said traits.  This activity just described causes a connection between the hyperstates of both of the said traits relative to one another --  to where the exterior counterpoise that holonomically binds the related codifferentiation among the two said traits produces a condition of hypnostates of the relatively holonomic ground states that are affiliated with the here mentioned general activity.  This will then cause a binary condition of an overall differentially singularized group state -- as the codifferentiation here bears a homotopy of an eigenbasis that is being collectively aquired in the general region.  Such an eigenbasis is partially differentiated upon by the quanta of a convergent overall norm-based projection that is here a reverse fractal of what is generally termed of as a norm-projection.  Sam Roach.    

A Description Of Doubolt Ghosts

A superstring may interact with another superstring in such a manner that the associated fields of the two said superstrings may travel in a relatively unitary trajectory in a collinear yet partially integrated and unitized curvature whose trajectory goes through an arbitrary Lagrangian directoralization through time. When such an interconnection of substringular fields binds with other of such cohomological multiplicitly stringular yet unitarily directoralized fields that are jointal to the arbitrarily initial discussed field, then the Ward Caucy association relating to the perturbation in Ward Neumman norm conditions causes an initially Imaginary Exchange in a reverse-fractored manner to the light-cone-gauge that settles into a unitary trajectory of field indices that organize into a set of spaces in terms of the Gaussian Conditions of each initially Rham trajectory that bear a different Kaeler Operation per space -- even though the unitized trajectory that moves as one unitary operation bears a group operational index that bears a group Hamiltonian eigenbasis. As the said Hamiltonian eigenbasis redistributes point particles and norm states via the holonomic phenomenology of the said Doubolt Space upon the said gauge actions just described, the resulting physical memory thus produced is a Doubolt ghost field whose Hodge Index in terms of a discrete ghost field of Doubolt cohomology may be described as an eigenstate of a Doubolt ghost anomaly. The integration of an entire eigenbasis of such eigenstates forms a region of Doubolt ghost phenomenology.