As to the Fractal of Magnetic Fields, Part One

Here is some of a heads-up as to the nature of the fractal of magnetic fields -- when one is to here consider some of the phenomenology that happens in the substringular.  Initially, the basis of the fractal of magnetic fields in the substringular is based, in part, on the multivarious conditions of the inter-relations of Fock Space.  This is due, in part, to the condition as to that -- the individual eigenstates of the wave-functionability of discrete energy permittivity is most directly associated with those individually taken eigenstates of superstringular counterparts that iterate just to the relative holomorphic side of the here multiplicitly taken eigenmembers of that holomorphic substrate, that acts as those superstrings of discrete energy permittivity that would here behave as the basis of the pointal-based conditionalilty of such a multiplicitly taken condition of discrete energy.  Just as the fractal of discrete electric field in the substringlar is based in part upon the angular momenta-based Hamiltonian-based operations of superstrings of discrete energy permittivity -- that of which may be here considered as being the fractal of discrete magnetic field in the substringular is based in part upon the spin-orbital-based Hamiltonian-based operations of superstrings of discrete energy permititivity.  So, since there are by far many more wave-like mini-stringular-based segments of core-field-density that are extended from that phenomenology that acts as the holonomic substrate of the counterparts of superstrings of discretely-based energy -- such a so-eluded-to Ward-Neumman-based physical bounds of the here multiplicitly taken counterstringular phenomenology may be then here considered to bear more of a shell-based piecewise continuous-based nature than that phenomenology that may be, instead, extrapolated upon a physical consideration of the Ward-Neumman-based physical bounds of the here multiplicitly taken superstringular phenomenology that I have here recently eluded-to as being the pointal basis of discrete energy permittivity.  So, the literal superstrings of discrete energy permititivity act more like a particle, and, the directly corresponding counterstrings -- of which iterate just to the relatively holomorphic side of these so-stated superstrings -- act more as waves (in comparison).  Since the counterparts of superstrings work in so as to behave in more of a shell-like manner -- in a direct comparison to the here so-mentioned particle-based holonomic substrate-based phenomenology of discrete energy permittivity -- the resultant Clifford-based Expansion that would thence be propagated from the kinematic and Laplacian-based extensions of such waves, that would then be protruded, over the projection of there exterialized trajectory, will inevitably tend to reach an assymptotic substringular Ward-Caucy bounds, work to form at least some sort of a homogenous slope, of which would eventually indirectly work to cause part of the reason as to the activity of the space-hole, this "space-hole" of which is what I term of as that general  activity that happens to the discretely ensuing kinematic superstrings and counterstrings of discrete energy permittivity -- during the majorization of what I term of as the Bases  of Light, in which the ultimate fractal of pressurized vacuum that exists in-between the superstrings and their correlative counterstrings works to cause those minute homotopic changes right before the quaternionic-instanton-field-impulse, that are needed in order for the holonomic substrate-based conditionalities of norm-based conditions to be able to change.  To Be Continued!  Sam.

Part Three of Session 9 of Course 18

When one is dealing with first-ordered point particles in the substringular, one is dealing with condensed oscillation of mini-string or condensed oscillation of core-substringular-field-density -- that would here come together in a form that one may say acts like a  "ball of yarn" of the just-mentioned condensed oscillation -- in so as to form a given arbitrary degree of a compactification of the so-stated local multiplicitly torsioned core-field density, in so as to form one immediate eigenmember basis of what may be either termed of as a point commutator that would here work to form a superstring, or as a point commutator that would here work to form a superstringular counterpart.  So, when one is dealing with the extension of mini-stringular segments that are jutted-out from any given first-ordered point particle, that would here work to form a ground-based superstring of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out from the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point particles that work to form the same respective directly associated given arbitrary superstring, and, to the most adjacent first-ordered point particle of the directly corresponding counterstring of discrete energy permittiivity -- one is then  here working with only one of such jutted-out mini-stringular segments.  Yet, when one is, instead, dealing with the extension of mini-stringular segments that are jutted-out from any given arbitrary first-ordered point particle, that would here work to form a Fock-based superstringular counterpart of the wave-functionablitiy of discrete energy permittivity -- besides those other given arbitrary mini-string segments that jut-out form the so-stated first-ordered point particle, in so as to work to interconnect the said point commutator to both the adjacent first-ordered point partictles that work to form the same respective directly associated given arbitrary counterstring, and, to the most adjacent first-ordered point particle of the directly associated superstring of discrete energy permititivity  -- one is then here working with many of such jutted-out mini-stringular segments.  The orientation of any given arbitrary first-ordered point particle to its surroundings, where it is positioned in its neighborhood, and, the pointal localization of the said point -- when this is taken relative to its environment -- is the basis for a respective fractal of electric field.  The coordinates that make it a field are the single wave propagations that are extended from the just so-eluded-to substringular neighborhoods.  To Be Continued!  Sam.

About the Transference of Third-Ordered Schwinger Indices

So, how do third-ordered Schwinger Indices become taken out of their directly corresponding respective light-cone-gauge eigenstates -- into the general Ward-Caucy bounds of the directly correlative Rarita Structure eigenstates?  Let me start to explain this here.  Initially, the gauge-bosons of the second-ordered light-cone-gauge eigenstates that work to comprise one unique respective given arbitrary first-ordered light-cone-gauge eigenstate "pluck" the here so-eluded-to second-ordered light-cone-gauge eigenstates, in so as to form the three-hundred third-ordered Schwinger Indices that would here be directly corresponding to the operational Hodge-based interplay of the here mentioned and eluded-to first-ordered light-cone-gauge eigenstate, that works to form the wave-functionability of the discrete energy impedance of one discrete unit of energy in time and space.  During the first six hbar increments of one iteration of group instanton -- of which would here directly correspond to the gauge-metrical activity that happens during one unit of BRST -- the so-stated "plucking" of the second-ordered light-cone-gauge eigenstates works to form third-ordered Shwinger Indices that start to vibrate at their general loci along the topology of the holonomic substrate of the said light-cone-gauge eigenstates.   These just eluded-to vibrational oscillations that work to perturbate the just mentioned eigenstates of the wavefunctionability of discrete energy impedance, immediately upon virtual resonation, are pulled by core-field density -- in a general directoral wave-pull, that is directed outward from the general locus of the here respective Ward-Neumman bounds of the directly correlative first-ordered light-cone-gauge, that is directly associated with the substringular holonomic substrate of discrete energy of the so-eluded-to general locus.  Right at the point that the initial 6 hbar increments of Real Reimmanian-based time of the correlative iteration of the corresponding instanton have elapsed, the so-stated third-ordered Schwinger Indices have reached the relative exterior of the Ward-Neumman bounds of the directly corresponding first-ordered light-cone-gauge-based substringular neighborhood.  This is simultaneous -- as is according to the vantage-point of a central conipoint -- to when the very end of BRST has just come to completion.  This is, as well, simultaneous -- as is according to the same just mentioned vantage point (of a central conipoint) -- to the ending of both the Polyakov Action and the Bette Action of the directly corresponding discrete energy of this case, at the so-mentioned specific locus at hand.  So, for the last (2pi-6) hbar increment of Real-based time, for the so-stated third-ordered Schwinger Indices, these vibrational oscillation-based indices are then made to inact a relatively high projected kinematic-based torsioning upon the surrounding Rarita Structure eigenstates -- over the course of the very ending of the directly corresponding duration of such a case of group-instanton -- in so as to work, per each successive iteration of instanton, at forming a sequential series of interactions of discrete energy upon gravitational-based strings, over time.  This is part of as to why we, as humans, tend to only perceive of the instant that happens right at the ending of BRST.  This works in so as to form that scalar attribute of the Rarita Structure eigenstates upon superstrings of discrete energy -- in the process of working to make what is known of as the Ricci Scalar to take effect, so that  there may be a covariant, codeterminable, and a codifferentiable manner as to the relationship between discrete energy and gravity itself.
To Be Continued!  Sam Roach.