Noether-Based Reverberation

How about if we chose the initial conditions of one respsective given arbitrary orbifold eigenset, to be of an accelerating nature -- as it is gradually increasing in its Noether Current, which is as the directly corresponding tense of its correlative Majorana-Weyl-Covariance is to here, as well, be going through a Ward-Caucy-based tense of a correlative gradual state of a gradual loosening of the directly corresponding cohomological inhibition of the said orbifold eigenset.   This orbifold eigenset is to act as if it is of the conformally invariant condition of the integrative Hodge-based Fourier-related behavior, that is of those eigenindices that are to work here as the resultant metrical-gauge-based Hamiltonian operation, that is of the Gliosis-based interdependent group-field of the correlative sum of the discrete quanta of energy that has then come together -- in so as to work to form the directly associated group of superstrings of such a given arbitrary respective case scenario. This happens in so as to operate, to help form one overall group-related function.  Let us next consider, that, after a relatively transient set of a sequential series of group-related instantons, that the so-stated orbifold eigenset of this case, is to make a Gliosis-based contact with an external field -- to where the said eigenset is to then act in such a manner, in so as to reverberate back into the opposite direction that it was initially traveling through.  Let us say, that upon the immediate Yukawa-based contact of the so-stated orbifold eigenset with the said external field, that this so-stated field will then work here as a barrier -- that is phenotypically to remain relatively stationary upon contact, to where it may be deemed that both the directoral-based topological sway, and also the directoral-based sum of both the angular momentum and the spin-orbital momentum of each of the individually taken discrete quanta of energy -- that work here, in so as to help to form the behavior of that tense of the respective given arbitrary Majorana-Weyl-Covariant-Mode, to where the correlative orbifold eigenset is to reverse in direction, via the reformation of its operational indices --to where those respective functional operations, that had worked to initially helped to form the Ward-Caucy conditions that had initially worked to form the initial so-stated Noether Current, is to then be reversed in its course of action, yet, with both an identical reverse-holomorphic topological wave-tug/wave-push, as well as being drawn into the same course of the gradual loosening of the respective tenses of its correlative Majorana-Weyl-Covariance.  This will then work to form a gradual increase in the directly associated Noether Current, -- yet both from the opposite end of the directly affiliated and so-eluded-to semi-infinite Real Reimmanian quantum well, as "well" as then working to help to cause the then accelerating orbifold eigenset, to then go from the initial rate that the said eigenset had been initially extrapolated at as, although in this case when going from the relatively opposite end of the quantum well, towards the relatively initial end of the said quantum well.  After the said orbifold eigenset is to susequently strike the initially so-eluded-to end of the quantum well -- which was that extrapolated end to where such a case was to have its initial instant under consideration at -- to where this whole process is to then reiterate.  One may then call such an iterative process -- a Noether-based reverberation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Noether Current And Acceleration

Let us consider an initial situation, as to a given arbitrary orbifold eigenset -- that is to have one respective given arbitrary Hodge-Index as to the quanta of discrete energy that work to comprise the said orbifold eigenset.  Let us say that the said eigenset is to be of a Calabi-Yau nature.  This would then mean that the so-stated orbifold eigenset would be of a mass-bearing Ward-Caucy-based condition.  The said eigenset is here to maintain the so-eluded-to tense of its Hodge-based indices, as well as its other general features, over the course of what is to here happen.  Let us say that the said respective tense of the condition, as to the Majorana-Weyl-Covariant-based mode of the said eigenset, is to gradual loosen -- as the orbifold of such a case is to respectively and consequently increase in its rate of transference, from one given spot to another.  This would then mean that the directly corresponding Noether Current is to gradually increase, as the correlative tense of its directly corresponding Majorana-Weyl-Covariance is gradually loosened.  It is this just mentioned general course of Fourier-based activity, that works to accelerate the so-stated orbifold eigenset.  As the so-eluded-to Calabi-Yau-related mass-bearing entity is to decrease in its cohomological-based inhibition -- its Majorana-Weyl-Covariance is to decrease in its scalar amplitude, and consequently, both the scalar amplitude of the correlative Noether Current of the said orbifold eigenset is to increase, and the velocity of the correlative orbifold eigenset is to increase as well -- which would here work to accelerate the so-stated respective given arbitrary orbifold eigenset, over its correlative group-metric.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

Noether Current And Velocity

When one is to have one given arbitrary combination of discrete quanta of energy, to be put together in one respective given arbitrary spatial arrangement -- with the proscribed Hodge-Indices as to the quantity of both the one-dimensional superstrings of discrete energy permittivity with their correlative substringular counterparts and the two-dimensional superstrings of discrete energy permittivity with their correlative substringular counterparts, that help to work to make-up the physical composition of one respective given arbitrary orbifold eigenset, as well as with the proscribed Hodge-Indices as to the quantity of both the respective and the correlative light-cone-gauge eigenstates and the respective and the correlative Fadeev-Popov-Trace eigenstates that work to form the discrete energy impedance that acts in so as to help make-up the physical composition of one respective given arbitrary orbifold eigenset -- then, one is to have the general format as to what the holonomic substrate of the phenomenology that you are looking for is. If such a substringular arrangement is in such a position, in so as to exhibit one specific given arbitrary tense of Majorana-Weyl-Covariance -- to where this is to work to form a specific effectual Noether Current that bears a resultant topological sway in one given arbitrary directoral-based translation, and if the tense of the vibration of the directly affiliated superstrins is to be of a Calabi-Yau-based nature, in so as to work at helping to form a Calabi-Yau manifold, then, this just described substringular arrangement will tend to form a respective given arbitrary mass, that will work to bear a velocity that will go in the direction of the directoral-based propagation that is of a state of optimum rest, -- for the so-eluded-to composite mass of the so-eluded-to substringular entity of such a case scenario.  To the extent of the lack of cohomological-based inhibition that the just described substringular entity is to have, on account of a respectively loosened tense of the correlative Majorana-Weyl-Covariance, --  the greater that the tendency will be, as to either the scalar amplitude and/or the scalar magnitude of the here directly pertinent Noether Current will be.  The greater that the Noether Current is, per the directly associated amount of substringular phenomenology that is to be transferred from one spot to another, the greater that the velocity of such a substringular phenomenology will then tend to be.  So if two different orbifold eigensets are to work to bear two different quanta of Hodge-based indices, yet are to still  bear the same eigenbase of Noether Current, in such a manner in so as to both be moving in the same Ward-Caucy-based directoralization of topological sway at the same time, via the vantage-point of a central conipoint -- then, that respective orbifold eigenset of such a case, that is to bear the smaller of the two so-eluded-to sets of Hodge-based indices, will then tend to travel at a faster velocity, over the directly associated group-metric that works to inter-bind the two said orbifold eiegnsets in both a codeterminable, a codifferentiable, and in a covariant manner, over time.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Exterior-Based Noether Currents

Let us say that one were to have a given arbitrary orbifold eigenset that was vibrating at one general spot, while it is as well remaining relatively still in a state of conformal invariance -- while, there are here to be certain individually taken orbifolds, that are to then exist from within the premises of the initially so-stated orbifold eigenset, that are definitively moving around from within the Ward-Caucy bounds of the relatively steady-stated externally-based orbifold eigenset-based reference frame of such a respective given arbitrary case scenario.  Since the externally mentioned reference frame -- being the said orbifold eigenset that is relatively stationary, is in a tense of conformal invariance, it is to here bear a Noether Current that works in such a cyclical-based manner -- to where the velocity of the so-stated reference frames as to being of the orbifold eigenset, may be equated to be at roughly zero, when in terms of the said external reference frame to here be staying from within an allotted specific zone of a vibratory tense of spatial parameters, over the directly affiliated group-metric of such a case.  Yet, since the orbifolds that are to here exist in a Fourier-based manner from within the said orbifold eigenset, are to here work to bear a definitive velocity during the so-eluded-to directly affiliated group-metric -- the individually taken orbifold eigensets that are to here be moving in both a definitive transversal and in a definitive radial-based manner over time, are to here bear a definitive Ward-based velocity, and thus, such so-stated internally-based orbifolds are to then bear such a relatively looser tense of a Majorana-Weyl-Covariance, to where such internally-based orbifolds are then to act in such a manner in so as to have a certain tense of a Noether-based current.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel Roach.

More As To Relativity Versus Noether Current

A mass is a discrete quantum of certain substringular Hodge-based indices, that work to inter-relate a respective given arbitrary quantity of the holonomic substrate of a Ward-Caucy-based condition -- that is of a set of one or more proximal localized cites, that are of the centralized knotting of a set of one or more Rarita Structure eigenstates -- that, when this is coupled with the Fourier-based activity of the force of gravity in general, this works to form that condition that one could call weight.  The increased or decreased thrust of an orbifold eigenset, is directly associated with the respective loosening or tightening of the correlative given arbitrary condition of the here proximal local tense of the Majorana-Weyl-Covariance, that is of the correlative specific substringular cite of such a respective region.  As a mass-bearing orbifold eigenset of discrete energy permittivity is to move, via a general directoral-based Lagrangian path -- through a correlative Hamiltonian operand, the resulting speed in a direction of the here pertinent orbifold eigenset, or, in other words, the resultant sequential series of the so-eluded-to delineation-based kinematic activity of the said orbifold eigenset -- as it is being translated spatially via the directly corresponding respective flow of its effective Noether Current -- will tend to form open-looped fermionic superstrings of discrete plain kinetic energy, in general, to the square of the resultant effect of the delineatory index, that is of the so-stated orbifold eigenset -- in its resultant directoral-based wave-tug/wave-push, that is Yukawa upon the Ricci Scalar, as the mass that is moving, is to bear its effect of its centralized knotting, that is upon the here local and pertinent eigenstates of the Rarita Structure.
I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.

As To Noether Current And Relative Velocities

Since the superstrings that work to comprise one given arbitrary orbifold eigenset, tend to be set in such a manner, in so as to conform to the same tense of a delineatory index -- such discrete quanta of energy permittivity are then to be set to conform to the same tense of one specific velocity, since any of such a respective given arbitrary orbifold eigenset, is a set of one or more discrete quanta of energy that operate in so as to perform one specific given function.  Since all of the superstrings and their correlative substringular counterparts, that work to make the phenomenology of the holonomic substrate of one said orbifold eigenset, are all traveling in such a manner -- in so as to work to produce an effect that is to conform to basically the same general velocity -- as these are all operational as a group, all of both of the directly corresponding superstrings and their correlative superstringular counterparts,that are of such a respective case, will then work to bear a resulting similar tense of both the same general scalar magnitude of Lorentz-Four-Contraction, as well as then working to bear the same general scalar magnitude of the directly corresponding Polyakov Action eigenstate.  This would then mean that all of the superstrings that work to help comprise one given orbifold eigenset, will bear one specific Noether Current -- that is to then be viable upon the delineatory index, that is correlative to the Fourier-based translation of one given arbitrary orbifold eigenset, that is here to be moving at a constant rate, in what is to then be exhibited in one specific tense of scalar amplitude or in one specific tense of scalar magnitude, -- over a directly corresponding sequential series of group-related instantons.  On this account, as the Noether Current of one orbifold eigenset is to be held constant -- then, the resultant velocity of the directly corresponding orbifold eigenset, will then be able to be extrapolated as being as well, held constant.  When there is an external Fourier-based action, that is to bear a Yukawa Coupling upon any given arbitrary respective orbifold eigenset -- this will tend to work to alter the Noether Current that is to then be exhibited by the correlative orbifold eigenset.  As the Noether Current of any of such a given respective orbifold eigenset is to then be altered -- then, this will tend to alter the Hamiltonian-based velocity of the said given arbitrary orbifold eigenset.  So, as the tense of the scalar amplitude of the Majorana-Weyl-Covariance of any given arbitrary orbifold eigenset, is either to be loosened or tightened in two different reference frames that are of both a mutually covariant and of a euclidean-based nature, over time -- this will tend to cause a respective acceleration or deceleration of the Noether Curent of the so-stated orbifold eiegenset.  As the said orbifold eigenset is either being accelerated or decelerated, over time -- the relative velocity of the so-stated orbifold eigenset is to then tend to be respectively accelerated or decelerated, over the said period of time of such a respective case.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Part One of the Eighth Session of Course 16

There are different types of periods within time that are essential for the existence of space and time.  What this means is that there are countless gauge-metrics -- both individual motions of eignestates of holonomic substrate of metric-gauge, as well as group metrics that integrate duration-wise, in so as to act within a discrete unit of time -- that occur within any given arbitrary individual duration of group instanton.  The course of group instanton -- which is mainly comprised of eigenstates of BRST -- is the general format of a discrete unit of time.  This is because we are only able to directly detect any given arbitrary motion in equal to or more than one integer-based multiple of group instanton.  Group instanton is the multiplicit-based integration of the condition of instanton, that is applicable to the reiterative basis of the delineatory and redelineation of substringular phenomena -- as this so-stated phenomena is fretted from one established framework of covariant, codiffereniable, and codeterminable distribution eigenbasis, that goes from one spot and one cohesive differentation -- toward the ensuing sequential series of distribution eigenbasis.  This is an eigenbasis that here appertains to the kinematic format of motion of the directly corresponding substringular discrete phenomena.  Such phenomena are thence pulled into those kinematic inter-relations that work to form the condition of both perpetual and sustainable energy in the multiverse.  It is the motion of the inter-relationship of the mutivarious and multiplicit substringular phenomena -- that occurs during the generally unnoticed iterations of Ultimon Flow -- that are not bound in a static-based framework, that works to help determine the directly corresponding covariance of the multiplicit delineatory bases of superstrings as a whole.  Such bases operate as an integrative set of Hodge-based Hamiltonian tensoric eigenstate of kinematic Gaussian spaces, that more directly work to control the perturbation of the general index of the Majorana-Weyl-Covariance of space-time-fabric -- in so as to allow for the existent flow of the general pattern of kinematic change, that works to allow for the continued multiplicit motion that is essential in order for energy to continue to exist.