Sets Of Inter-Laced Braided Steady-State Electrostatic Eigenstates -- Not Super-Conformally Invariant -- Force Fields

 Force-Fields are sets of inter-laced braided steady-state electrostatic eigenstates, that are Not super-conformally invariant at an internal reference-frame. TO BE CONTINUED! SINCERELY, SAM ROACH.

Norm-State-Projections And Schwinger-Indices

Those Schwinger-Indices, that are formed by the plucking of second-order light-cone-gauge eigenstates by their directly corresponding gauge-bosons -- flow along the Rarita Structure.  As such said Schwinger-Indices flow along the Rarita Structure, part of their correlative activity -- is to work to vibrate the multiplicit holonomic substrate of norm-state-projections.  As such said Schwinger-Indices work to vibrate the multivarious holonomic substrate of norm-state-projections, -- this general genus of a Fourier-related activity, works to help at influencing the multiplicit genus of force that is to be exhibited at different substringular loci, as this is here to be taken all along the overall said Rarita Structure.  This, then, works to help at influencing as to whether a specific Ward-Cauchy-related locus --  is to be working to exhibit either the strong force, the electrostatic force, the gravitational force, and/or the weak force.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

The Third Part Of Session Three Of Course 20 -- Calabi Interactions

Light that is moving through a pure vacuum, tends to be propagated in a straight line.  This, however, does not take into consideration the generally mild influence, that the force of gravity works to impose upon the propagation of electromagnetic energy.  Space-Time-Fabric is not perfectly straight -- it is curved, -- and such a tendency of space-time-curvature, tends to be basically due to the direct influence of gravity upon physical phenomenology. The force of gravity is a significantly weaker force than the electrostatic force.  This is why  -- when the respective gravitational force is of a relatively low level of scalar magnitude -- the influence of gravity upon light, does not have very much of an effect upon both how "straight" and how "fast" that the said light is being propagated in a pure vacuum.  Yet, when the force of gravity is of an extremely strong scalar magnitude -- such as with a black-hole -- then, any proximal local light will bend, due to the so-eluded-to gravitational force of such a case, to where the correlative electromagnetic energy will not even be able to escape the then eminent condition of being bent into the so-stated given arbitrary respective black-hole of such a case scenario.  Furthermore -- the more physically isolated that any given arbitrary beam of light is, from other physical phenomenology in outer space, -- to where the then directly corresponding gravitational force is basically null upon such a respective beam, -- then, the less influenced that the said beam of light will be, from being neither bent at all nor slowed at all by the correlative force of gravity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Current And The Polyakov Action

The higher that the tense of the scalar amplitude of an eigenstate of the Polyakov Action is, in any given arbitrary respective case scenario -- at one given cite, to where this is happening among discrete energy quanta, -- the more overtly that the directly corresponding mini-stringular segmentation is to then be fed into the general arena, in which the directly corresponding light-cone-gauge eigenstates are to be at.  The more overt that the directly corresponding holonomic substrate-related quanta, that is of mini-stringular segmentation -- is to be, in terms of the scalar magnitude as to the amount of that mini-stringular segmentation that is to be fed into the given arbitrary respective general arena, where the directly corresponding light-cone-gauge eigenstates are at, the lower that the frequency will tend to be, as to the vibrational oscillations that are of the nature as to the condition of what the directly affiliated Schwinger-Indices will correspondingly happen to be -- at the correlative respective region, that is most associated with the said discrete quanta of energy impedance -- that are to be acting here in a tightly-knit Fourier-based manner, that is to here be both Yukawa to the directly corresponding superstrings that are to here be proximal localized -- in so as to work to form discrete energy permittivity, as well as this is to also be acting in a tightly-knit Fourier-based manner that is Gliosis to both the directly associated light-cone-gauge eigenstates, as well as here being Gliosis to the directly affiliated Fadeev-Popov-Trace eigenstates.  Things tend to bear more of an active charge when these are in motion.  This is the general condition as to what happens in a relatively comparative case, when the correlative Lorentz-Four-Contractions of a given arbitrary respective case scenario, are anywhere from barely existent down to being null --  at the so-eluded-to general substringular locus that is in question here.  This works to explain, as to the tendency of there being comparitively relatively less  charge at a general locus -- that works to bear little to no Lorentz-Four-Contraction, or, in other words, this works to explain as to the tendency of there being relatively less of a general condition of charge at a general substringular locus, that is basically stuck at that moment in a tense of a relative condition of Majorana-Weyl-Invariance.  When there is a relative surplus of mini-stringular segmentation, that is here to be fed into the general Gliosis-based light-cone-gauge-affliated field -- at a specific general locus, during BRST, then, this works to help to form a relative condition of there being an added attenuation of the superfluities of the directly corresponding eigenstates, that are of the centralized knotting of the here pertinent Rarita Structure eigenfield.  This said attenuation of such a surplus -- that is to be existent at the so-stated or the so-eluded-to nodes, works here to help to cause a relative decrease or depletion of the torsional eigenindices -- that would otherwise be delineated more heartily by the overall Hamiltonian momentum (both the spin-orbital and the transversal components combined) of the pertinent twisting of the cites of the directly corresponding eigenstates that are of the so-stated centralized knotting of the Rarita Structure.  This is what works to help to cause the tendency of any entity -- that is of a relatively low velocity-based mode, -- to tend to bear relatively less of an electrostatic charge, than it would otherwise have, if it were to bear more of a substantial velocity over time,  that would otherwise be spontaneously extrapolated in such a case.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.