Tightly-Knit Holomorphic Transfer

Let us initially consider two different cohomology-related mappable-tracings -- of which are here to be correlative to those world-sheets, that are to be of the paths of two different respective individually taken kinematic orbifold eigensets, -- that are here to bear a tense of trivial asymmetry, when this is here to be taken as an overall interdependent Yukawa-related relationship, that is of both a covariant, a co-determinable, and of a co-differentiable nature.  Let us next consider, -- that there is here to ensue, the Gliosis-based activity of a group-attractor, that is here to work to form a general spontaneous activity -- that is to result in a general manipulation of the topological manifold of the earlier inferred set of trivial asymmetric world-sheets, by which the the initially mapped-out interdependent Lagrangian-based paths, are then to work to bear a helical-related tensor, that is to be consequently imparted upon the topological surface of the tracings of the said world-sheets, at a level that is Poincare to the surface, that is immediately external to the shell of the core-field-density of the path-based cohomology-related eigenstates, that work to form the world-sheet-related physical memory of those orbifold eigensets, that had just tread upon the herein inferred proximal local Hamiltonian operand.  The more tightly-knit that the holomorphic transfer is to be, of the inferred interdependent covariant-related helicity, that is here to work to inter-bind the so-eluded-to trivial asymmetric path-like entities, the greater that the scalar amplitude will tend to be, of the helical twisting, that is here to be of the Yukawa-related coupling of the two said asymmetric paths. Therefore; the less tightly-knit that the holomorphic transfer is to be, of the inferred interdependent covariant-related helicity, that is here to work to inter-bind the so-eluded-to trivial asymmetric path-like entities, the less great that the scalar amplitude will tend to be, of the helical twisting, that is here to be of the Yukawa-related coupling of these two said asymmetric paths. To Be Continued!  Sincerely, Samuel David Roach.

Added Dimension Of Torque To i*PI(del) Action

Let us initially consider a mass-bearing orbifold eigenset, that is here to be undergoing a course of a Noether-related flow, that is smoothly changing in its relative motion in its relationship with electromagnetic energy, in both a transversal and in a radial manner -- over time.  This added tensor of an additional change in motion when in relationship to light, will consequently work to cause an added effectual spatial dimension of delineation, to the correlative multiplicit placement of the directly corresponding partition-based discrepancies, per each individually taken superstring of discrete energy permittivity that works to comprise the said orbifold eigenset, that are here to be smoothly delineated -- per said inferred superstring, -- over the mappable-tracing of the contour of the Laplacian-related topological stratum, that works to comprise their holonomic substrate, -- in a slightly different manner per each successive iteration of group-related instanton, over a sequential series of such said respective instantons -- as to where the associated flow of the correlative i*PI(del) Action, will consequently work to bear an added spatial dimension of angular momentum-related torque, over the course of such an inferred binary perturbation in the directly associated Lorentz-Four-Contraction, that is here to be changing in both a transversal and in a radial manner simultaneously -- via the vantage-point of a central coniaxion.  Sincerely, Sam Roach.

A Little More As To Lagrangian Versus Metrical

Let's initially consider the fundamental condition, that a superstring is a discrete quantum of energy permittivity.  Its motion through a path is its Lagrangian.  The relationship of the direction of the wave-tug/wave-pull of the dimensional-related directorals, that are of the said superstring, when this is taken in a correspondence with its heading, over a relatively considered holomorphic direction over a set duration -- is the metric of a superstring.  In a very real way -- both a Lagrangian-based tense of a Chern-Simons singularity and a metrical-based tense of a Chern-Simons singularity, are related to the pulse of a Ward-Cauchy-based phenomenology.  The main difference is -- that a Lagrangian-related Chern-Simons singularity tends to happen when a quantum of discrete energy is to alter relatively abruptly in the conveyance of the motion of its energy over time, -- whereas, a metrical-related Chern-Simons singularity tends to happen, when a quantum of discrete energy is to alter in its dimensional-related direction -- as a velocity-based tensor relative to light, over a sequential series of correlative group-related instantons.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Part Two Of Bundles Of Covariant Energy

Let us consider two different sets of orbifold eigensets -- that are to interact here, in a manner that is to be both covariant, codeterminable, and codifferentiable, -- as the two said given arbitrary orbifold eigensets are to act as two tenses of energy, that are to interact in an interdependent manner, over a relatively transient duration of time.  Let us next consider one of the two mentioned orbifold eigensets as being of a vector-based bundle, whereas, the other of the two mentioned orbifold eigensets is as being of a tensor-based bundle.  The orbifold eigenset that is to work to bear a vector-based bundle of cohomology, is to act in so as to exist in a tense of superconformal invariance -- to where the so-eluded-to cohomology that is thus formed by the Fourier-related differentiation of the said orbifold eigenset -- is to be of a Rham-based cohomology.  The orbifold eigenset that is to work to bear a tensoric-based bundle of cohomology, is to act in so as to exist in a tense of bearing a relative lack of superconformal invariance -- to where the so-eluded-to cohomology that is thus formed by the Fourier-related differntiation of the said orbifold eigenset, is to be of a Doubolt cohomology.  Such a dual state of the resultant activity that is here to happen, due to the interaction of the two said orbifold eigensets -- as these two sets of superstrings are to traverse through their correlative Fourier-related transforms -- may then be said to bear a tense of tending to bear a state of behaving in manner that is partially Yau-Exact, over time. I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.