External Cohomological Shell

When one is to extrapolate the detection of any stratum of a mass, -- one will tend to be extrapolating the electrons of the directly corroborative mass -- since it is the electrons that are of the atoms that are here in so as to work to make-up such a said mass, that act in so as to surround the nucleus of those just mentioned atoms, that are here to comprise the phenomenology of such a mass.  Furthermore -- when one is to extrapolate the detection of any given arbitrary superstring, -- one will tend to be extrapolating the externalized core-field-density of the innermost cohomological stratum, that is just outside of the holonomic substrate of the topological surface that is of such a superstring, when this is taken at the Poincare level, -- since it is such a general genus of an innermost cohomology, that works to act as a physical memory of such a string, in so as to work to act as a tangible "handle" of phenomenology, by which such a superstring may possibly be apprehended in at least some manner shape or form.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Homology Versus Cohomology

Here is the basic difference between what a homology is, versus what a cohomology is:
A homology is the physical memory as to the when, the where, and the how, that either an open substringular strand or an open substringular loop has differentiated, as a Hamiltonian eigenindex, over time.  A cohomology is the physical memory as to the when, the where, and the how, that a closed substringular loop has differentiated, as a Hamiltonian eigenindex, over time.  Such physical memories may be anywhere from being at a proximal locus, that is just external to the core-field-density of the superstring -- in other words, at the Ward-Cauchy-based field that is just external to the topological stratum of the substringular eigenindex, -- to being as a physical memory that may be extrapolated from the effect of such a respective strand or a loop, that has here to have just potentially differentiated through a Lagrangian that may be mapped-out, over a Fourier Transform that involves a sequential series of instantons.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

A Description Of Campbell Ghosts, Part Two

Now, I will continue with the suspense. A discrete homeomorphic set of such a redistribution and re delineation of point commutators, that are inexact and non linearly based, on account of the motion of Campbell states, forms a physical memory of where and how such Campbell norm-states differentiated kinematically over a certain given Fourier Transformation. Over the course of one discrete instanton, such a discrete field of physical memory as considered over the Laplacian metrical delineation that is used to consider the differential geometry of the composition of such a discrete ghost defines a ghost anomaly of a Campbell norm-state. The covariantly related Laplacian Field that defines the cohomology of inter related adjacent Campbell ghosts is used to consider and classify the eigenbasis of a Campbell norm-state ghost region. So, the partial differentiation that is used to determine one Campbell norm-state discrete ghost field may be integrated in certain cohomological point commutator Fock regions to determine the Laplacian eigenbasis of such related fields as well as to determine the Fourier Transform eigenbasis of such a prior named field when considering such a field's kinematic operation when taken over a sequential series of instantons. The aberration of the homeomorphic topology of such an eigenbasis forms pseudo-real permutations of such an integrative multiplicit ghost field on account of other gauge-metrics that occur over a transient period. Please study what I have just written, and e-mail to me your thoughts about this!
Sincerely,
Sam.