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.