Some Stuff As To Space-Time-Fabric

Mini-Stringular Segmentation works to form those general fields, -- by which discrete energy and norm-state-projection-related commutation, are thence to be able to be held together, via what may be termed of here as being the general substringular condition of "homotopy." In-Between the countless eigenstates of mini-stringular segmentation, that are here to be existent in the substringular, -- there is the multiplicit proximal local presence, of what I term of here, as being the phenomenology of "pressurized vacuum."  The overall arena, by which the substringular is here to be exhibited by discrete energy -- over the course of the sequential series of the countless iterations of those instants, of what I term of as being the generally noticed durations of Ultimon Flow, there tends to generally  be the condition, by which such an arena is here to be filled by the summation of both the overall scalar magnitude of mini-stringular segmentation, Plus, the overall scalar magnitude of that pressurized vacuum, that is here to exist in-between the strand-like eigenstates of the said mini-stringular segmentation. I will continue with the suspense later! To Be Continued! Samuel David Roach.

Annharmonic Vibration And Tachyonic Flow

So -- if one given arbitrary superstring of discrete energy permittivity, is to both vibrate annharmonically in an odd number of spatial dimensions in a holomorphic manner right before an iteration of BRST, --  as well as vibrating annharmonically in an odd number of spatial dimensions in an antiholomorphic manner during the immediately ensuing iteration of the directly corresponding Regge Action eigenstate, -- then, that respective given arbitrary superstring will then tend to become tachyonic.  When one or more superstrings are to become tachyonic -- then, these will undergo at least a moment of tachyonic flow.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

Solution 5 Of Test 2 Of Course 20

For the first 384 iterations of group-related instanton, once a photon has directly struck another discrete quantum of energy, the scattered photon, when individually taken, is entropic -- and it is then said to temporarily bear an abelian light-cone-gauge topology.  This means that the mini-stringular segmentation of the correlative Kaluza-Klein topology, is relatively supplemental and not sinusoidal.  This is due to the condition, that the said entropic photon is here to bear a "spring-like" reflexive nature -- that may here to attributed to the directly corresponding kinematic activity of the holonomic substrate of the so-eluded-to light-cone-gauge eigenstate, in so as to respond in a homotopic manner, is so as to not shatter upon a Gliosis-related contact.  When electromagnetic energy scatters upon a phenomenon, individual photons strike the externalized core-field-density of individually taken light-cone-gauge eigenstates.  Likes repel -- in part due to that adjacent phenomena that are of the same electrostatic general nature, must spin in an assymetric manner -- relative to one another.  The said "springing" of the light-cone-gauge eigenstates of photons, works to allow for photons to repel what these had struck directly.  So, the thence straightened-out nature of the overall mini-stringular segmentation of the light-cone-gauge eigenstates of electromagnetic energy -- when these scatter upon something -- works to allow for the need for a very transient repulsion of electromagnetic energy from what it had just directly contacted, as it basically is a fractal of what would happen as is according to the Pauli-Exclusion Principle.  The "counter string" of discrete energy permittivity, that would here be as is directly corresponding to the here so-eluded-to superstring -- along with the mini-stringular segmentation that works to inter-bind the said counter string with its correlative superstring of discrete energy permittivity, -- acts as a physical buffer to the spring-like action, that is of the light-cone-gauge topology of a photon.  I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.

Field Genus And Tendency Of Holomorphic Direction

Over the course of any one iteration of group-related instanton -- an f-field is an f-field, a d-field is a d-field, and a p-field is a p-field.  Yet -- over the course of any one iteration of group-related instanton -- there are often superstrings of an f-field, that may be influenced by an external source, in so as to work to bear a tendency of holomorphic topological sway, that may either be in-between the normal directoral tendency of an f-field and the normal directoral tendency of a d-field, or in-between the normal directoral tendency of an f-field and the normal directoral tendency of a p-field.  Likewise, there are often superstrings of a d-field, that may be influenced by an external source, in so as to work to bear a tendency of holomorphic topological sway, that may either be in-between the normal directoral tendency of a d-field and the normal directoral tendency of an f-field, or in-between the normal directoral tendency of a d-field and the normal directoral tendency of a p-field.  Likewise, there are often superstrings of a p-field, that may be influenced by an external source, in so as to work to bear a tendency of holomorphic topological sway that may either be in-between the normal directoral tendency of a p-field and the normal directoral tendency of an f-field, or in-between the normal directoral tendency of a p-field and the normal directoral tendency of a d-field.
I will continue with the suspense later!  To Be Continued! Sincerely, Samuel David Roach.

As To The Kahler-Metric And The Polyakov Action

In any given arbitrary case -- the tendency is, to where, given that there is the same scalar amplitude or the same scalar magnitude of the Polyakov Action for one bosonic superstring of discrete energy permittivity, when taken versus another of such individually taken bosonic superstrings of discrete energy permittivity -- the condition exists, to where the more that the Kahler-Metric is Yukawa to any of such a said respective given arbitrary superstring, -- the more that the tendency is, to where there is to then be more of a scalar amplitude of mini-stringular segmentation, that is to be thus fed into the proximal locus of the field of such a so-stated respective superstring, over the course of any single respective given arbitrary iteration of BRST, in which such dual Ward-Caucy conditions are to be thus compared.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Test Solutions For Test One of Course 4 on the Globally Distinguishable Vs. the Substringular, Part Three, by Samuel Roach

11) A point particle generally travels in the "current" of a majorized plane of multiplicit Minkowski space. A majorized plane has four dimensions as a minimum. A Fock point particle is 10,000 times from being completely condensed, and a stringular point particle is two times away from being completely condensed. 10^4 = 10,000. So, a Fock point particle exists in its whole region by iterating in 10,000 different spots per 10,000 radial motions of the said point particle as it travels through iteration and Ultimon time (the "time" in between iterations). This means that a stringular-based point particle exists throughout its neighborhood by a factor of 5,000 per 10,000 radial motions of the said particle as it travels through iteration and Ultimon flow.



12) Waves are expelled and brought in by first-ordered point particles to allow for the differentiation of mini-string, or, in other words, to allow for the motion of substringular fields. If substringular fields did not move, strings wouldn't move and would cease to exist.



13) The computer is an example. IF THEN ELSE statements.



14) The motion and holonomity of point particles as part of superstrings during discrete units of time is detectable by discerning the activity of the said superstrings over the course of a Fourier Transformation.



15) Electrons exist in D-fields, which are six-dimensional. These have six-dimensions that they exist in because an electron, in order to have both angular momentum and spin-orbital momentum that are crossed relative to each other by the "right-hand-rule" must exist in a double supremumized kinematic differentiation relative to the first-ordered point particles that comprise the superstrings of the said electrons.

Course 3 on Lorentz-Four-Contractions, Session 14, Part 1

The appearance of stringular contraction is in the globally distinguishable. You may wonder, "What does he mean by detecting a string within a neighborhood as it is iterating and reiterating several times?" Since a string is a small phenomenon that is of itself a vibration of several point particles that comprise its make-up, then, as a string defines its position as what it is for just a moment, it is iterated. Change is constant. The strings existence as a string in a specific position as being exactly what it was during the metric of pointal organization that allows it to be that is basically no longer than the instantaneous organizational moment that it takes for the points to become "exact" and "linear" when considering the basis of a 1-D string or a vibrating strand, form an instanton-quaternionic-field-impulse range right before this iteration, and then dissociate after this iteration. So stringular organization is only a transient thing when considering ultimon flow. Yet, if you detected a "string" at any spot, it would show a sense of stability in terms of empirical reality, even though it would indicate a condition of vibration. How? When a string in the globally distinguishable appears to be basically vibrating as a still phenomenon, then the substringular action indicates motion of the string that keeps coming back to basically the same spot if in a state of superconformal invariance. Since the string keeps approximating the same position here after it keeps returning after circling the Continuum each time, it appears to be basically changeless in terms of Cartesian displacement as a unit. The condition in the lateral displacement of the string as a unit is the condition of a phenomenon that does not differentiate kinematically as a unit in the globally distinguishable. I will appease the suspense of my readers by providing more knowledge of this session later.

Test 2 of Course 2

Test 2 of Course 2

1)What is the difference between the stuff inside of a point particle and the stuff that it gives off?

2)What is the difference between the point-fill of a stringular point particle and the point-fill of a Fock Space point commutator?

3)What is the function of a point commutator?

4)What is the difference between a string, and a globalization of point commutators?

5)What is Fock Space?

6)What exists between Real & Fock Spaces?

7)What is the space-hole?

8)What type of commutation exists between both sides of the space-hole?

9)Describe as thoroughly as you can what happen to a string in general in-between iterations.

10)What geometric disposition causes point commutators to tag along dissociated strings?

11)What is the difference between a regular phenomenon and homotopy?

12)What is the difference between a discharge and delineation?

13)Name an example of a phenomenal discharge.

14)Name an example of a homotopic delineation.