When Gliosis to The Kahler-Metric

 Pure energy is not literally 100 percent efficient. When a given arbitrary Hamiltonian Operator is to be Gliosis to the Kahler-Metric, those individually taken discrete energy quanta, of which are here to work to comprise such a stated Hamiltonian Operator, are to work to bear a dimensional modification, of which is here to work to allow for the re-attainment of the optimum utilization, that is directly associated with the herein inferred net discrete energy quantum (of which is here to be referring to the said Hamiltonian Operator). TO BE CONTINUED! SINCERELY, SAMUEL ROACH.(1989). 

Spurious Dimensional Gauging -- Metric-Related Chern-Simons Singularities

 When the dimensional gauging of a Hamiltonian Operator becomes spurious, it will spontaneously tend to consequentially work to bear a correlative set of metric-related Chern-Simons singularities. SAM.

Spurious Dimensional Gauging

 When the dimensional gauging of a Hamiltonian Operator becomes spurious, its pulsation will tend to become spurious. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (1989).

As To Metric-Related Pulsation

 A binary metric-related pulsation, often tends to have a deeper dimensional pulsation, than an otherwise analogous unitary metric-related pulsation; A tertiary metric-related pulsation, often tends to have a deeper dimensional pulsation, than an otherwise analogous binary metric-related pulsation, etc. ... Sincerely, Sam. 

A Refinement -- As To Metric-Based Chern-Simons Singularities

 When a cohesive set of one or more discrete energy quanta, is to alter in its dimensional-related pulsation, As this is here to be considered, -- over a sequential series of group-related instantons -- this general process of a superstring-related activity, -- as taken at the locus at which such an alteration in the dimensional-related pulsation is here to be occurring, is thence to be indicative, of the proximal local presence, of a tense of a metric-based Chern-Simons singularity. TO BE CONTINUED! SINCERELY, SAMUEL ROACH. (1989).

Dimensional Compactification And Lowered Charge

Since when a mass-bearing orbifold eigenset is to bear basically the same tendency of motion, -- except for the general attribute, in which there is to be a situation, that is appertaining to the manner in which there is here to be a change in the set of physical conditions, that is here to be most directly associated with a dimensional compactification in the metric-related gauging of such a cohesive set of discrete energy quanta, -- to where such a change in the physical conditions of the behavior of this said cohesive set of discrete energy quanta, is to result in the tendency of a decreased scalar amplitude in the rate of the perturbation of its directly associated Chern-Simons Invariants -- that, this will consequently tend to reverse-fractal into the covariant proximal local decrease in the scalar magnitude of the charge, that such an inferred orbifold eigenset will then ensue to be exhibiting. To Be Continued! Sincerely, Samuel David Roach.

Yukawa Versus Gliosis To Kahler-Metric

Any given arbitrary superstring that is not frayed, is always going to be Yukawa to the Kahler-Metric, yet, only when such a so-eluded-to superstring is in the process of working to attain those fractals of discrete energy that these need -- in order to both persist and exist as discrete energy -- will such superstrings actually be Gliosis to the Kahler-Metric.  The metric of a superstring of discrete energy permittivity, is its dimensional-related pulsation.  Any superstring that is not being frayed, will always work to bear a dimensional-related pulsation over time.  Yet, such an eminent tendency of a superstring to work to bear any of such a tense of a dimensional-related pulsation -- works to bear a general condition, to where, since any given arbitrary respective superstring is not literally 100 percent efficient in the "real world," discrete energy must recurrently, over time, go through a "renovation-like" process of such a prior inferred re-attaing, of those fractals of discrete energy -- to where discrete energy is to thence to be put into such a condition-related "position," to then to be able to reattain the ability to work to bear one manner or another, of a dimensional-related pulsation over time.  This process of such a said "renovation-like" activity, is when discrete energy -- after a set of iterations of the ending segments of the contingent correlative group-related instantons, in which such discrete quanta of energy are to interact directly in a Gliosis-based manner, with a respective tense of an eigenstate of the holonomic substrate of the Klein Bottle, is to happen, in order to both modulate the morphology-related qualities of the said discrete quanta of energy, and also in so as to modulate the wave-tug-related qualities of the same said discrete quanta of energy -- so that the said stringular-like phenomenology that is here to thence to be made Gliosis to the Kahler-Metric, is to both reattain its efficiency and its "stamina," over time.  Furthermore, such a said process -- works to make it easier for abelian groups to latch-on, in an indistinguishably changing manner, to the externalized shell of the multiplicit topological proximal region, -- in so as to work to help at making the functioning of cohomological attainment to be able to be possible, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Dimensional Change And Singularities

Let us initially consider that general Ward-Cauchy-related set of conditions, that are appertaining to spatial dimensionality, that is to be considered for one given arbitrary superstring of discrete energy permittivity -- that is Not in consideration of what is to otherwise be in a directly correlative relationship with the Ward-Cauchy-based conditions of Beti numbers, (to where this is not here to be directly considering what happens, right before and right after each of such iterations of BRST) -- but, instead, to where this is to be taken in a directly correlative relationship with the Ward-Cauchy-based conditions that are here to be during each sequential iteration of BRST -- over an evenly-gauged Hamiltonian eigenmetric.  Let us then say, that for the just mentioned superstring of discrete energy permittiivty, over the course of each iteration of BRST that is here to be correlative to the said evenly-gauged Hamiltonian eigenmetric -- that the here mentioned superstring is to oscillate back-and-forth, from being a two-dimensional spatial entity into being a three-dimensional spatial entity.  Let us next say that the general holomorphic direction of the said string, is here to be maintained -- over the set framework of time.  Since the just so-eluded-to back-and-forth alteration in spatial dimensionality, is here to alter the directoral-related flow of the said string's directly corresponding angular momentum eigenindices -- such a back-and-forth alteration in the directly corresponding dimensions of the spatial parameters of the said string, will then tend to alter the dimensional-related direction of the holonomic substrate of the correlative string in and of itself, at the Poincare level to the topological surface of the directly corresponding superstring of discrete energy permittivity, during each succeeding iteration of BRST for such a said string.  Such an alteration of dimensional-related direction for the holonomic substrate of a discrete quantum of energy, will then tend to work to form the presence of metrical-related Chern-Simons singularities over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

A Llittle Bit More As To Conformal Dimension

A physical dimensionality, for all intensive purposes, is discrete -- when one considers the number of spatial dimensions plus time. Yet, if you want to get technical, since superstrings bear discrepencies that I term of as partitions, the conformal dimension of a superstring is never precisely One or Two, respectively. The conformal dimension of a one-dimensional superstring will vary -- depending upon the discrete truncation as to the scalar amplitude of the given arbitrary degree of Lorentz-Four-Contraction that would here correspond. If a one-dimensional superstring is "contracted" by a factor of two to just under three, then, it will have 15*10^7 mentioned partitional discrepencies along its topological contour. Yet, if a one-dimensional superstring is "contracted" by a factor of 3*10^8, then, it will have only one mentioned partitional discrepencies along its topological contour. The conformal dimension of a superstring with two of such partitions will be 2^((15*10^7)/10^43)). A similar situation is true for two-dimensional superstrings, except, a bosonic superstring also has one of such partitons, if it is going at the speed of light. (Only bosonic strings can travel at exactly the speed of light.) Also, if a superstring has two of such partitions, its conformal dimension will be 1+2^((15*10^7)/10^43). As an ansantz, 2^((15*10^7)/10^43) is basically one, since any number to the zero power is one. Although, a swivel-like-shaped superstring is more likely to become unoriented at the Bette Action, and, therefore, it is more likely to become tachyonic than if it were shaped otherwise. To Be Continued.