Ghosts Of Orbifold-Based Phenomena

When  physical spaces -- in the form of  orbifolds and/or orbifold eigensets -- are pulled through dual discrete Lagrangians, whether or not the just mentioned general format of the respective singular Lagrangians are unitary, binary, or overtly multiplicit in directoral-based permittivity, the so-stated orbifolds and/or orbifold eigensets will form ghost anomalies as these move through the corresponding Hamiltonian-based operands of physical space in which the said orbifolds and/or orbifold eigensets move through here.  Such individual respective Hamiltonian-based operations will here involve the multiplicit formation of potentially many ghost anomalies that come together in a group-based cohomology that will here form, in so as to map-out a tracing as to the relatively recent physically-extrapolatable memory of where, how, and when an orbifold and/or an orbifold eigenset had been kinematically displaced and delineated over a sequential series of group instantons -- the physical memory of an orbifold and/or an orbifold eigenset when relative to one or more other orbifolds and/or orbifold eigensets.  Given the substringular environment that exists after an arbitrary discrete physical space has moved in so as to form a trajectory of its kinematic projection over time, the ghost anomalies that are thus formed may be anharmonically scattered at any time, once the corresponding mapping of the correlative group-based world-sheets have been traced-out by the harmonic scattering of the here given arbitrary relatively forward-holomorphic moving norm-states that get in the path of the motion of the corresponding superstrings that work to comprise the eluded to orbifolds and/or orbifold eigensets.  If such ghost anomalies are formed between two or more orbifolds and/or two or more orbifold eigensets that are Njenhuis in terms of their kinematic-based covariance towards each other over the same group metric, then, the ghosts that these form will tend to be Njenhuis relative to one another. Yet, if such ghost anomalies are formed between two or more orbifolds and/or two or more orbifold eigensets that are Real Reimmanian in terms of their kinematic-based covariance towards each other over the same group metric, then, the ghosts that these form will tend to be Real Reimmanian relative to one another.  Often, though, the residue that is formed by the anharmonic scattering of different sets of ghost anomalies that are initially of different universes may be brought into a closer Reimmanian inter-relationship towards each other after the corresponding recycling of their respective mini-string segmental partials have been recycled through enough times.  I will continue with the suspense later!  Sincerely, Sam Roach.