Sound/Heat -- Group-Attractors/"Ghost-Based Inhibitors"

 The phenomenology of sound, as incurred upon a group of Noether-Based mass-bearing cohesive sets of discrete energy quanta, when done in the right manner, may often have the general potential tendency, of having the capability, of working to form a set of one or more, of what I have termed of as being, the general phenomenology, of "group-attractors." Whereas; The phenomenology of heat, as incurred upon a group of Noether-Based mass-bearing cohesive sets of discrete energy quanta, when done in the right manner, may often have the general potential tendency, of having the capability, of working to form a set of one or more, of what I have termed of as being, the general phenomenology, of "ghost-based inhibitors." I WILL CONTINUE WITH THE SUSPENSE LATER! SINCERELY, Samuel David Roach.

Group-Attractors -- Wess-Zumino Interactions

When a set of Ward-Cauchy-Related group-attractors, are to work to form a Wess-Zumino interaction, that is here to be incurred upon the kinematically covariant radial Lagrangian-Based spin-orbital motion of a molecule, to where such a molecule, is here to be in the form of a an integrable arrangement of Noether-Based mass-based cohesive sets of discrete energy quanta, this general process, will thereby consequently tend to result, in a harmonic flow of radial-based vibrations, to where this will often tend to help at working to form a tense of sound. TO BE CONTINUED! SINCERELY, SAMUEL DAVID ROACH. (PHS1989).

Certain Eminent Presence Working To Produce Cohomology-Related Generation/Degeneration

When there is an eminent Yukawa-related presence of group-attractors, that is here to be relatively proximal local to the kinematic formation of a mappable-tracing of cohomology-related eigenstates, -- this general type of a substringular process, tends to work to help in producing a state of cohomology-related generation.  Consequently; when there is an eminent Yukawa-related presence of ghost-based inhibitors, that is here to be relatively proximal local to the kinematic formation of a mappable-tracing of cohomology-related eigenstates, -- this general type of a substringular process, tends to work to help in producing a state of cohomology-related degeneration. Samuel Roach.

Dirac Effect Of Group-Attractors Upon Ghost-Based Inhibitors

Let us initially say, that one is here to have a given arbitrary mass-bearing orbifold eigenset, -- that is here to be acted upon, by both a set of group-attractors & a set of ghost-based inhibitors.  The Fourier-related activity of such a so-stated set of group-attractors, is then in this particular case, to tend to work to bear a Dirac effect upon the Fourier-related activity of such a so-stated set of ghost-based inhibitors.  Sam.

More As To The General Way Group-Attactors Act

Superstrings that are to be brought together, in so as to operate to perform one specific function -- are brought into an eminently Yukawa Coupling, by the Fourier-related activity -- of what may here be termed of as group-attractors.  I will continue with the suspense later!  To Be Continued!
Sincerely, Samuel David Roach.

Perturbative Cohomological Eigenstates

Besides the more obvious general reason as to why an initially Rham-based cohological eigenstate, is to be perturbated into the ensuing general tense of a cohomological stratum, that is known of as a Doubolt cohomology, -- as to when a Rham cohomology is to scatter upon another cohomology, in such a manner that the initially mentioned Rham cohomology is to then to tend to become, instead, of the said Doubolt-related nature, -- there is as well to be one other epifany-related additional general alterior reason -- as to why an initial Rham cohomology is to eventually become of a Doubolt nature, to where this is because of the eventual spontaneous proximal local presence of certain entities, which may be as both group-attractors and/or the proximal local presence of certain entities, which may be as ghost-inhibitors, -- to where both of such just mentioned general categories of what would generally be as the nature of being Cevita-related Hamiltonian operators, are here to have an eminent tendency of, via the innate Hamiltonian operation of the activity of their respective Fourier Transforms, to helping at causing a peturbative effect upon both the pulsation and/or the path-based flow of the so inferred orbifold eigenset, that  was to initially be functioning as a Hamiltonian operator that was here to be undergoing a Fourier Transform -- via the mappable-tracing of the initially mentioned Rham cohomology, that is here to be extrapolated as to then of becoming of a Doubolt cohomology, over an evenly gauged  Hamiltonian operation.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Fourth Part Of Cyclical Reverberations And Reference Frames

Let us initially say that one is dealing with the situation which is as before -- to where there is a respective given arbitrary orbifold eigenset, that is to here be reverberating in a cycle -- in which the said orbifold eigenset is to be moving at the so-eluded-to relatively internal reference frame, via a relatively rectangular Lagrangian-based path that is cyclical permutative -- in such a manner to where it works here in so as to bear a Fourier-based turning at each corner, to the relative left or Njenhuis-to-forward-holomorphic direction, to where, from a relatively external reference frame, the so-stated set of superstrings that are here operating in so as to perform one specific function, is, as well, reverberating back-and-forth in a cycle that goes from moving into the relative "up" or norm-to-forward-holomorphic directoral-based path, into then going into a motion that is then going into the relative "down" or norm-to-reverse-holomorphic direction, and back again, -- to where the so-stated relatively external-based flow, is to here act in a tensoric-based manner, when this is in a direct relationship to the here more relatively internal-based flow. As said before, -- those group-attractors that act upon the said orbifold eigenset -- in so as to help to work to cause the said eigenset to move into the said relative "up"-based direction, act upon the said orbifold eigenset in a relatively chiral-related manner, -- whereas contrariwise, those group-attractors that act upon the said orbifold eigenset in so as to help to work to cause the said eigenset to move into the said relative "down"-based direction, act upon the said orbifold eigenset in a relatively antichiral manner.  The general effect of the just mentioned chiral-based influence, that is of this particular case, will then tend to work in so as to help to form a scalar magnitude of those certain directly corresponding torsional eigenindices, that will then tend to bear the index-based existence of singularities that will have Real Reimmanian roots, whereas, in contrast, the general effect of the here mentioned antichiral-based influence of this particular case, will then tend to work in so as to help to form a scalar magnitude of those certain directly corresponding torsional eigenindices, that will tend to bear the index-based existence of singularities that will have complex roots.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cyclical Reverberations And Reference Frames, Part Three

Let us initially consider a given arbitrary orbifold eigenset, that is moving, as mentioned before, via a rectangular Lagrangiain-based path -- in such a manner, as to be tending to turn at each correlative corner, towards the relative left.  Let us, as before as well, consider that the said orbifold eigenset is to here work to bear cyclic permutations.  Let us then, as well, consider that the said orbifold eigenest is to, from an external reference frame, be reverberating -- as well -- from going towards the relative "up" (norm-to-forward-holomorphic) to going towards the relative "down" (norm-to-reverse-holomorphic) direction -- in so as to iterate through such a so-eluded-to cyclical path, as a phenomenology that is to reverberate via a binary-based genus of a tensoric-related Lagrangian-based path, over time.  Let us next consider those correlative group-attractors -- that work in so as to help in the influencing of such an orbifold eigenset, to be able to undertake such a back-and-forth reverberation -- that is to here reiterate in such a relative "up-to-down" associated manner.  Those group-attractors that would work here -- in so as to influence such an orbifold eigenset to move into the relative norm-to-forward-holomorphic direction -- would here tend to have a chiral effect upon the holonomic substrate of the said orbifold eigenset, over a sequential series of instantons.  Contrariwise -- those group-attractors that would work here in so as to influence such an orbifold eigenset to move into the relative norm-to-reverse-holomorphic direction -- would here tend to have an antichiral effect upon the holonomic substrate of the said orbifold eigenset of such a case, over a sequential series of instantons.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.