Heat -- Chern-Simons Invariants -- Entropy

 The less infrared photons (heat) that are to be proximal local to the region of field, that is here to be immediately external to the core-field-density of a charged mass-bearing cohesive set of discrete energy quanta, the less anharmonic metric-gauge-related eigenstates that will consequently tend to be emitted, via the directly associated perturbation in those given arbitrary Chern Simons Invariants, that are here to be exhibited, in the general process by which the said mass-bearing cohesive set of discrete energy quanta, is here to tend to work to bear a tense of spin-orbital oscillation, as its is here to be transferred along its course in the arena of space-time-fabric, -- since a relative decrease in temperature, will consequently tend to work to decrease the entropy that is here to be emitted by the motion of such an inferred charged particle. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAM ROACH.

Light Into Kinetic Energy

 When a given arbitrary superstring, of a discrete quantum of electromagnetic energy permittivity, as exemplified  by the particle-related nature, of the holonomic permittivity of a photon, is to spontaneously convert into a superstring of discrete kinetic energy permittivity, — this general process, acts as the Inverse Operation, of the Fujikawa Coupling via the Green Function. Sincerely, SAM ROACH. (1989).

Vibrational Source Of The Forces Of Nature

 Just as the light-cone-gauge is the vibrational source of the reductional forces of nature, the multiplicity of the countless individually taken gauge-bosons, are the particle-related source of the reductional forces of nature. Gauge-Bosons work to "pluck" their directly corresponding second-order light-cone-gauge eigenstates, in so as to work to form a tense of Schwinger-Indices. This just mentioned general genus of Schwinger-Indices, in turn, propagate outward, in so as to convey those vibrational states, that operate in so as to work to allow for both the existence and the perpetuity of these herein inferred general forces of nature. I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach. (1989).

Holomorphic Direction And Light Scattering

When an individually taken photon is to scatter upon another discrete quantum of energy, not only will the photon alter here in its holomorphic direction, once it is to become scattered into an entropic phenomenon -- it will temporarily alter in its holomorphic tendencies, until it is here to become re-quantized into a beam of electromagnetic energy.  You see, every different general genus of Ward-Cauchy-related phenomenology, works to bear its own set of holomorphic tendencies.  A discrete quantum of energy that is of a d-field is to work to bear a different set of holomorphic tendencies than a discrete quantum of energy that is of an f-field - whereas, a discrete quantum of energy that is of a p-field is to work to bear a different set of holomorphic tendencies than a discrete quantum of energy that is of either a d-field or of an f-field.  Furthermore, -- a discrete quantum of energy that is of a scattered photon as it is of an entropic state, is here to work to bear a different set of holomorphic tendencies than those of an unscattered photon that is not of an entropic state.  This is due to the basic general condition, -- that both the wave and the particle-based characteristics of a discrete quantum of energy, that are of a given arbitrary general genus of a Ward-Cauchy-related field -- are going to vary, when that said general genus of a field is to alter -- which is here going to mean, that the wave-tug/wave-push of such a field is going to then to tend to be inherently exhibited differently.
I will continue with the suspense later! To Be Continued!  Sincerely, Samuel David Roach.

Hamiltonian Operations Of Gravity

Often, superstrings of a Hamiltonian operation of gravity, may simultaneously (via the vantage-point of a central conipoint), act as both a graviton and a gravitino.  This is when a Ward-Cauchy-based particle of a Hamiltonian operation of gravity, is to bear both radial and transversal characteristics, over the course of the same distinct iterations of group-related instanton.  So, let's say that, over the course of one specific iteration of instanton, that a Ward-Cauchy-based gravitational particle is to be at both one positioning of a fractal of angular momentum and at one position of a fractal of spin-orbital momentum.  Next, at the ensuing iteration of instanton, the just mentioned particle is to be distributed in such a delineation -- to where its fractal tense of angular momentum had to have just altered by one Planck Length, while its fractal tense of spin-orbital momentum had to have just altered by one Planck Radii.  Let us next say that the just mentioned tendency, is then to re-occur for a significant number of iterations of group-related instanton.  A graviton is a superstring of a Hamiltonian operation of gravity, that works to involve the transversal motion of the so-eluded-to eigenstate -- whereas, a gravitino is a superstring of a Hamiltonian operation of gravity, that works to involve the radial motion of the so-eluded-to eigenstate.  One could then say, when such a just mentioned gravitational particle is to display both a transversal and a radial motion -- over the same general tendency of motion -- that it is to act as both a graviton and as a gravitino simultaneously (via the vantage-point of a central conipoint).  One could then say, that such a particle may be considered as a unitary dual-state of gravitational eigenstate, that is to exhibit the gauged activity of both a fractal tense of angular momentum and the gauged activity of a fractal tense of spin-orbital momentum -- over the course of the same evenly gauged Hamiltonian operation.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Topological Sways That Bear Freedom Of Motion

Let us here first consider a theoretical substringular particle, that moved in the relative holomorphic direction in only one spatial dimension, over time.  The particle that is moving such, will then be of either zero spatial parameters of dimensionality or of one spatial parameter of dimensionality. Its motion would the, in this theoretical case, of a Fourier-based kinematic displacement, that would form a flat Lagrangian path as a Wilson Line -- that is being delineated as a propagating Hamiltonian index, over a sequential series of instantons.  Let us next theoretically consider an either zero-dimensional , or a one-dimensional or a two-dimensional particle that is moving homomorphically as a line that curves as is the piecewise continuous intrinsic curvature of space at each so-eluded-to individually taken point -- in a plane that is of only two spatial parameters of dimensionality, plus time.  Its motion will then tend to work to bear a topological sway, that will here have its bearings in the alterior spatial dimension that is normal to the intrinsic dimensional parameter that it is moving through.  Next, let us theoretically consider an particle that has a dimensional set of parameters that work to include up to three spatial dimensions plus time.  It is moving relatively flush in the relative holomorphic direction.  Its topological sway will then tend to bear a binary Laplacian-based coniaxial of motion -- as the said particle is moving as is the intrinsic curvature of space at each individually taken piecewise continuous iteration of instanton, in which the particle moves into the Lagrangian path of its given arbitrary Hamiltonian operand, over time.  Take this pattern.  If one had a particle that traveled in a 32 dimensional volumed space over time -- but flush in the relative holomorphic direction -- then, its topological sway may work to include a 31 dimensional coniaxial that is normal to the so-stated Lagrangian-based path of the said holomorphic-based motion of the particle here that is moving in 32 spatial dimensions plus time.  Two of the said coniaxials of this topological-based sway of this latter case will be of a Real Reimmanian-based nature, and, the other 29 coniaxials of this topological-based sway of this latter case will be of a Njenhuis-based nature.  To Be Continued!  Sam Roach.