Toroidal-Shaped Cohomology-Related World-Sheets -- Gliosis-Sherk-Olive Ghosts

 Mass-Bearing superstrings of discrete energy permittivity, tend to work to form toroidal-shaped cohomology-related world-sheets. World-Sheets are the projection of the trajectory of discrete energy phenomenology (superstrings). Cohomology may be perceived of, as being of the eminent topological substrate, of the core-field-density of discrete energy quanta. What I worked to describe of, during some earlier times in my blog, as being "ghosts," -- were actually what I meant to describe of, as being "cohomology-related eigenstates." I referred to such said "eigenstates," as being of a ghost-like nature, since the actual specific phenomenology that I was here to be referring to, is of a constantly indistinguishably different nature. (To where, although these "appear" to be consistently spontaneous latched upon eigenstates, that are stable in super conformal invariance at a covariant locus, in time and space, the specific phenomenology that is here to be latching, at the inferred covariant respective loci, are to constantly be of different actual "stuff.") Those ghost-like phenomenology, that are here to be directly appertaining, to the multiplicity of the toroidal-shaped topological manifolds, that are here to be directly associated with those  respective cohomology-related world-sheets, that are here to be formed by the resultant projected trajectory, of mass-bearing superstrings of discrete energy permittivity, may be described of here, as being of the general nature, of acting as, "Gliosis-Sherk-Olive" ghosts. (1989). SAMUEL DAVID ROACH.

The Annuli Of Toroidal-Related Cohomology

Mass-Bearing superstrings of discrete energy permittivity, tend to work to bear toroidal-shaped cohomology-related structures.  Such just stated toroidal-shaped cohomology-related structures, are directly associated -- with what may be termed of as being Gliosis-Sherk-Olive ghosts.  Toroidal-Shaped cohomology-related structures, tend to work to bear the proximal local physical presence of annuli -- that are here to be located at a the relative "center" of the stratum of their directly corresponding holonomic substrate.  As such said mass-bearing superstrings are to be moving at a higher rate, these just mentioned annuli, are to tend to shrink in diameter, in proportion to how the scalar magnitude of the directly corresponding Lorentz-Four-Contraction -- that is here to be effectual upon that multiplicit orbifold eigenset, that is here to be comprised of by those implied composite correlative mass-bearing superstrings of discrete energy, that are here to work to bear the attribute of the said multiplicit annulus at each of their relative centers, -- is here to be acting upon the relativistic Ward-Cauchy-related conditions of such an inferred set of discrete energy, that operate to perform one specific given arbitrary function.    So, if the Lorentz-Four-Contraction -- that is here to be acting upon any one given arbitrary orbifold eigenset, is to be of a scalar magnitude of "2," then, the diameter of each of the annuli of those cohomology-related structures, that are of those individually taken superstrings of discrete energy permittivity, that work to comprise such a said eigenset, -- will  consequently tend to be shrunk by a factor or "2," from the diameter that these would have theoretically had, at a relative terrestrial stand still. Sincerely, Samuel David Roach.

Ghost-Inhibitors And Ward-Polarization

Let us initially consider a set of both cohomological eigenstates and a set of cohomological eigenindices, that are here to be formed by the Fourier translation of the Lagrangian-based path of an orbifold eigenset over time.  Let us say that there is then to be a set of relatively reverse-holomorphic norm-state-projections, that are here to work to bear a Gliosis-based contact upon the so-eluded-to ghost-based indices of both the said cohomological eigenstates and the said cohomological eigenindices -- that I had earlier mentioned to have just been formed over time.  Let us next say that such a said contact is to bear an eminent tense of Ward-Polarization -- that is Poincare to the topological surfaces of the cohomological states that are here to be struck in a relatively reverse-holomorphic-related manner, -- over the so-eluded-to proscribed evenly-gauged Hamiltonian eigenmetric.  Such a said activity will here tend to work to form a Rayleigh scattering of the implied ghost anomalies that had just been formed -- of which will then tend to annhamonically work to scatter such ghosts out of order in the process.  Such a set of relatively reverse-holomorphic norm-state-projections, will, in this particular general genus of a case -- act as ghost-based inhibitors.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

The Recycling Of The Residue From Annharmonically Scattered Cohomologies

In the process of the Fourier-related translation of Gaussian Transforms, -- the Rayleigh scattering of GSO cohomological eigenstates that are formed on the relative multiplicit Real Reimmanian Plane, works to form a general tense of Ward-Cauchy-related residue, that is replenished by that general tense of Ward-Cauchy-related residue, that is formed by the Rayleigh scattering of Neilson-Kollosh cohomological eigenstates, that are, instead, to be formed off of the relative multiplicit Real Reimmanian Plane.  This happens in such a manner, to where such residues act, in so as to work to form a tense of a system of substringular or Ward-Cauchy-related recycling, over time -- in so as to help-out in the process of that general multiplicit freeing-up of room in the substringular, that is needed in order for each eigenstate of Hamiltonian operation, to be able to both persist and exist, as eigenindices of discrete energy that act in so as to allow for both the persistence and the existence of energy at all.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Invariant Modes And Transiency Of Ghosts

The tighter that the Majorana-Weyl-Invariant-Mode is of an orbifold eigenset -- the longer that those directly corresponding cohomological-based tracings, that are formed as the ghosts or the physical memories of the motion of the directly associated orbifold eigenset -- that is of the so-eluded-to given arbitrary respective Majorana-Weyl-Invariant-Mode, tends to be.  Likewise, the looser that the Majorana-Weyl-Invariant-Mode is of an orbifold eigenset -- the shorter that those directly corresponding cohomological-based tracings, that are formed as the ghosts or the physical memories of the directly associated orbifold eigenset -- that is of the so-eluded-to given arbitrary respective Majorana-Weyl-Invariant-Mode, tends to be.  So, the tighter the Majorana-Weyl-Invariant-Mode is -- the less transient that its correlative ghosts tend to be, and, the looser the Majorana-Weyl-Invariant-Mode is -- the more transient that its correlative ghosts tend to be.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

Different Formats of Certain Ghost Anomalies

Initially, as I have mentioned before, the ghost anomalies or the  cohomological-based indices, that are formed by the mappable tracings of two-dimensional superstrings of discrete energy permittivity, tend to bear a relatively torroidal tense of morphology -- while, the ghost anomalies or the  cohomological-based indices that are formed by the mappable tracing of one-dimensional superstrings of discrete energy permittivity tend to bear a relatively conical tense of morphology.  So, Gliossi-Sherk-Olive ghosts tend to bear either a torroidal or a conical shape -- via the mappable tracings of their respective trajectory, over time.  Yet, the shape of a Neilson-Kollosh ghost takes a little bit more of an explanation to tell here.  In general, the shape or the morphology of a Neilson-Kollosh cohomological-based mappable tracing (one eigenset of the directly inferred general genus of such indices) will either tend to be the shape of an annulus of either  a converging or a diverging hyperbolically-shaped toroid, or, the shape of a Neilson-Kollosh ghost may often, instead, be of the outer perimeter of the Ward-Neumman bounds of the respective shape of an annulus of either a converging or a diverging hyperbolically-shaped toroid.
I will continue with the suspense later!  Sincerely, Sam 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.