When A Kahler Manifold Is Not Diffeomorphic

 When a Kahler Manifold lacks a “monomial” tense of a shape, it may be said to Not be diffeomorphic. Samuel David Roach. 

The more resolute that the cochain complex of a net cohomology-related eigenstate is to be, the more potentially embedded that its corroborative mappable-tracing will consequently tend to be.  

A strengthening of the net gauge-action, of an eminently corroborative, kinematically propagated, Kahler Hamiltonian Topological Manifold, may often tend to be capable, of working to enhance the Ward-Cauchy-Related structural integrity, of the covariant net topological stratum, that such an implicit team of cohesive discrete energy eigenstates, is here to work to comprise, as it is tugged along its Lagrangian.

A given arbitrary tense of a Fourier-Related-Progression, that is tugged through a relatively viscous heterogeneous state of space-time-fabric, will often tend to spontaneously become more anharmonic in perturbation, than if such an otherwise analogous tense of a Fourier-Related-Progression, is to be, instead, tugged through a relatively less viscous heterogeneous state, of space-time-fabric. 

When the interface that is to be kinematically developed, between a particle-like phenomenon, And, the eminently corroborative Higgs Field, is to bear a spontaneously perturbation, in its Stokes-Based Concavity, this general process, may often tend to potentially facilitate the reductional capacity, for the spontaneous generation of Imaginary Charge, as tending here to be holomorphic in delineation, as transmitted via a mass-based structure. 

When the motion, of an eminently associated, harmonic recursively reverberating, Kahler Hamiltonian Topological Manifold, is to bear a tense of conformal invariance, in so as to tend to exemplify, the general type of a certain static equilibrium, it will thereupon often render, here, that the eminently corroborative, indistinguishably different, effectual net Wick Action, that is here to spontaneously facilitate the ensuing generation of the Landau-Gisner Action, will often spontaneously tend to work to bear, an eminently associated, recursively reverberating, harmonic motion, via the equivocally necessary Ward-Polarization, of the said contingent Wick Action, in so as to effectively allow, for this harmonic case of super symmetry, to happen, as well as in a manner, that is vicariously gauged.

Part One Of Gravitational Topological-Variance

 When an electron is struck by a beam of electromagnetic energy, it (the electron), will tend to fall back-and-forth an energy level -- to where the resultant residual spare energy, that is here to be respectively incurred upon the covariant Ward-Cauchy-Related bounds of such a stated electron, is to consequently be released, as a tangentially propagated discrete quantum of electromagnetic radiation. Right around the moment, during which a beam of electrodynamic radiation, is initially to come into a direct contact, with the holonomic stratum of the core-field-density of an electron, (of which is to be about 7*10^(-17) of one second after the immediate Gliosis-Based contact), the interaction between the inferred beam of photons with the topological stratum, that is here to be of the core-field-density of the electron, to where the shape of the topological contour, of that gravitational field, of which is here to work to bear an eminently associated covariant immediately externalized relationship, with the topological field that is proximal local to the core-field-density of the herein stated electron, is to alter in its directly associated topological morphology, to where such an inferred gravitational field, that is here to be directly corresponding to the said electron that I have eluded to here, while in mentioning such a respective given arbitrary type of a case scenario, is thereby to consequentially vary in the delineation-related distribution of its directorial-related construction, to where such a general genus, of the correlative alteration in the directorial-related contour of such an inferred topological gravitational field, may consequently be said, to be undergoing the general process, of what I call, the reductional operational-related Ward-Cauchy-Related physical condition, of what may consequently be called, the Gravitational Topological-Variance. (GT).

Let us next say, that the electron-related co-tangential bundle that is being approached, by the earlier eluded-to beam of electrodynamic radiation, is here to be of an arbitrary spatial dimensionality, of N dimensions. (It may be anywhere from co-tangential bundle R3, to co-tangential bundle R6). The equation that I have recently come-up with, for working to help determine what the Gravitational Topological-Variance, is, for the case of an initially scattered electron, of which is here to be proximal local in its eminent presence, after about 7*10^(-17) of one second upon the initial immediate contact of the inferred electromagnetic energy with the eluded-to respective given arbitrary electron that is here to be beginning to be scattered, as taken at the Poincare level to the immediate region of direct interaction, is:

GT(v) = ~ {[[The Ricci Flow]*[((N-1)*e^((2*(1-N)) - 1]*[((N-1)*e^((2*(1-N)) +1]]

*(((N^.5)/N)*((e^(The Ricci Flow))^6) {+ - (I hat), + - (j hat), + - (k hat), ... + - ( q(n) hat)}.

To where, the "hat" term, is here to elude to a reference, to the reductional shape-based delineation-related distribution, that is here to be constructed, via an understanding of the Laplacian-Based direction(s), of which are here to be directly related to the mappable contour of the shape of the directly correlative gravitational field, that is here to be expressed, at the eminent proximal local region, that is immediately externalized to the core-field-density, that is here to be directly associated with the eminently correlative electron, that is here to be of such a respectively given arbitrary type of a case scenario. SAMUEL. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! 

More As To Holomorphic Direction

The holomorphic tendency of an orbifold eigenset, is associated with that tendency of direction -- in which an orbifold eigenset will most likely take -- when one is here to consider both the shape and the spatial dimensionality of the said orbifold eigenset.  To Be Continued!  Sincerely, Samuel David Roach.

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.