Reversal Of Relative Holomorphic Direction -- Fadeev-Popov-Trace Eigenstate -- Ward-Supplemental Alteration Of Flow

 When a given arbitrary Noether-Based Fadeev-Popov-Trace eigenstate, is to kinematically incur a coaxial tense of a reversal, in the flow of its covariant proximal local relative holomorphic direction, this will often work to allow for this inferred genus of a superstring-related operation, to often tend to help, in working to allow for the general means of a consequentially resultant tendency, in which the directly associated inferred respective discrete quantum of energy, of which is here to be corresponding, in an eminent correlation, to the initially stated respective given arbitrary Fadeev-Popov-Trace eigenstate, of such a particular case, to thereby have a relatively heightened probability, of consequently tending to work to bear an ensuing spontaneously occurring Ward-Supplemental flow, of its correlative cohesive integrable composite Noether-Based stratum of topological manifold. I WILL CONTINUE THE SUSPENSE LATER! TO BE CONTINUED! SAM.1989.

More As To The Workings Of Homotopic Residue

 Superstrings of discrete energy permittivity Want to move in a certain given arbitrary innate direction, -- When given What the specific traits and other physical attributes, that are of such an individually taken  respective given arbitrary superstring, are here to be, in such an eluded-to type of a  theoretical case scenario. That directly corresponding respective mass-bearing cohesive set of discrete energy quanta, of which the directly corresponding composite individually taken superstrings of discrete energy permittivity, are to work to comprise, tends to Want to move Into its relatively Innate Holomorphic Direction. All of the  "strings" of discrete energy permittivity, that are thenceforth to work to comprise the earlier mentioned respective cohesive set of discrete energy quanta, are to be delineated during the general course of group-related instanton, At the external shell of the said correlative cohesive set of discrete energy quanta, that these are here to take part in working to be exhibited at, when such an inferred type of a set of interdependent energy, that is here to be operating to display one specific task, is here to be considered -- as a metaphorical "team" of reductional energy. The cohesive set of discrete energy quanta of such a respective given arbitrary case scenario, is to take precedence, -- as to the resultant accommodation of its "phenotypical" display, as to its tendency, to move Into its innately holomorphic direction, -- to where the inferred "team" of energy, will consequently tend to "win-out," as to the ensuing resultant spatial direction, at which the inferred net composite energy-related quantum, of such a general tense of a case scenario, is thereby to be transferred into, over the span of a directly corresponding duration of discrete time. SAM.

Transversal-Related Drive; Spin-Orbital-Related Drive

The transversal-related drive of any given arbitrary orbifold eigenset, tends to be geared in the holomorphic direction -- that is most associated with the wave-tug of its angular momentum; And -- the  radial-related drive of any given arbitrary orbifold eigenset, tends to be geared in the holomorphic direction -- that is  most associated with the wave-tug of its spin-orbital momentum. Sincerely, Samuel David Roach.

Lorentz-Four-Contraction And Relative Length

Let us initially consider a mass-bearing orbifold eigenset to be moving, at just under the speed of light.  It's Lorentz-Four-Contraction, is here to be 3*10^8.  The given arbitrary respective orbifold eigenset, is here to be traveling in the relative forward-holomorphic direction.  The said eigenset is here to work to bear 3*10^8 times as much mass, than it would normally have, when at a relative terrestrial standstill.  This will then work to mean, that this said given arbitrary orbifold eigenset, is here to work to bear the proximal local presence, -- of 3*10^8 times as many mass-bearing superstrings of discrete energy permittivitiy, than it normally would have, if at a relative terrestrial standstill.  This will then work to mean, that such a said orbifold eigenset, is here to tend to be quite significantly denser, -- than it would otherwise be, if it were, instead, to be traveling at a much slower rate, in relation to the motion of light.  Since the said respective orbifold eigenset, is here to be much denser -- it is here to bear a much greater gravitational wave-tug, upon its immediate physical environment, at a level that is Poincare to the general spatially differentiable region, at which the inferred eigenset is to be moving through.  Since the said eigenset is here to work to bear a greater gravitational wave-tug for its size, it will consequently tend to work to draw its composite mass-bearing superstrings of discrete energy permittivity inward, in a euclidean manner, that is of a proportionality, that is correlative to the directly corresponding Lorentz-Four-Contraction.  This will thence, tend to work to make the length of the initially stated orbifold eigenset, -- when this is here to be taken in the holomorphic direction of its motion, that is here to be at just under light speed, -- to tend to bear a Lorentz-Four-Contraction, when this is taken in a relativistic manner to a terrestrial observer, to then become thinner, by a factor of 3*10^8.  I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

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.

A Basic Example Of Ward-Polarization

Here is a basic general example, of what may be termed of as a phenomenon -- in which there is to be the Ward-Cauchy-based condition of Ward-Polarization:

Let us initially say that one is to have an orbifold eigenset, that is to be undergoing a tense of conformal invariance at its internal reference-frame, that is here to work to bear a tense of what would here be at least the equivalence -- of a tense of angular momentum, that is subtended in what would here be the relative forward-holomorphic direction.  Let's next say, that over the translation of a relatively small distance, as taken in the earlier mentioned forward-holomorphic direction, from where the initially stated orbifold eigenset is to be bearing its so-eluded-to tightly-knit location of vibrational oscillation,  -- there is to be the bearings of a tense of a quantum of electromagnetic energy to be present.  However, there is here, in this general case, an orbifold eigenset, that is placed in-between the direction of the angular momentum that is of the initially stated orbifold eigenset and the so-stated quantum of electromagnetic energy -- that is here to be placed in such a manner, to where the relative holomorphic direction of the orbifold eigenset that is here to get in the way, is to be orthogonal to the holomorphic direction of the initially stated orbifold eigenset.  Such a substringular condition of such a case, may then work to partially, if not completely, block any otherwise eminent Yukawa Coupling to then to be able to be achieved, between the initially said orbifold eigenset and the so-eluded-to electromagnetic energy-based orbifold eigenset.  This general genus of a Ward-Cauchy-related condition,  is one of basically countless types of situations -- in which there is to be the phenomenon, of what may be termed of as Ward-Polarization.  Samuel David Roach.

Reverberations And Kahler-Metric eigenstates

Let us initially consider an orbifold eigenset -- that is reverberating back-and-forth at one given rate, over an initially transient group-metric.  Each time that the so-stated orbifold eigenset is to flip in its general holomorphic direction -- there is to be a proximal localized antiholomorphic Kahler condition.  This will then tend to work to lead into a Gliosis-based interaction of a Kahler-Metric eigenstate, with the said orbifold eigenset -- over an even more transient sequential series of instantons.  Let us say that the initially so-eluded-to rate of reverberation, is then to be sped up.  This will then tend to work to cause a heightened scalar amplitude of the rate, by which there are to be the resultant formation of the respective proximal localized antiholomorphic Kahler conditions.   This will thereby work to increase the scalar magnitude as to the  degree and/or the manner by which the proximal local Kahler-Metric, is to here be Yukawa to the said orbifold eigenset, over time.  Furthermore, if the so-eluded-to rate of the respective reverberation, is to instead be slowed down -- the resultant Kahler-Metric will then end-up, to bear less of a scalar amplitude as to the wave-tug of that respective general Yukawa Coupling -- that is to here be imbued upon the said orbifold eigenset, over time.  I will continue with the suspense later!   To Be Continued!  Sincerely, Sam Roach.

Course 5, Session 7, Part II

Now, to continue with the rest of Session 7 of Course 5. Counterclockwise unscrews, or brings reality toward its observer. The Creative Force needs to observe us. So, point commutators flow from right to left in the realm of the holomorphic direction in the course of forward moving time, and point commutators flow from left to right in the realm of the holomorphic direction in the course of backward moving time. Constant change forces life to learn. The basis of constant change is the basis of Organized Learning. In order for points to be points with discrepancies, constant compactified change must happen within a region small enough to where the translocation of its indices changes the operand of its surroundings. So, if a point is really a point, the region around it will exhibit a field. If the field exists, there will be an electric and a magnetic field associated with it on a fractally minute basis. Points are an approximate kinematic association. No lie. A point is a density of redistributed space that effects the area where it differentiates. As the point translocates, the ends of its condensed oscillation that comprise its make-up uncurl a little because of the fields of other points acting upon it, and the point prepares to interface with other of such point particles. What are these fields? Energy is everywhere. Energy and space are interchangeable. Point energy is dense energy that is compactified. When a magnetic and an electric field are formed, ripples in the energy between point particles forms a wrinkle in space-time fabric. These wrinkles act like hands that move to "try" to untie the ends of the strings at the ends of the said point particles. These oscillating wrinkles of space-time fabric are fields or field eigenstates. When these field eigenstates are kerneled to a specific tangent of the norm operator of one of these string ends, the point particles associated with this are contracted. If enough of these field eigenstates are kerneled as such, then the point particles' end points are pulled into the operand of space that is not dense. When the extent of continued pull brings two point ends to touch each other, then these come into contact and touch for a brief instant. As soon as the point ends curl around each other into a hooked normalcy, then the point ends pull each other straight and slip off of each other. This is since the elasticity of point particle end points have complete normalcy to all others that these come into contact with as these exhibit some sort of attraction that bends them like a supplemental compliment. (Normal Line).