Part Five of Session 8 of Course 9

The "flapping" of the Planck-Related phenomena that correspond to bosonic superstrings that bear a Kaluza-Klein light-cone-gauge topology is affiliated with the normalization of the Planck-Related phenomena that were just mentioned with the directly surrounding Planck-Related phenomena.  This is due to the condition of Gaussian-Based stability that is associated with any unperturbated orbifold and/or due to the condition of Gaussian-Based stability that is associated with any unperturbated orbifold eigenset.  The mentioned normalizations of the two categories of Planck-Related phenomena relative to one another is controlled by the flow of the substringular fields in the form of the flow of the negative norm-states and positive-norm-states and the zero-norm-states (Zero-Norm-states are isolated first-ordered point particles that, as is the case with all first-ordered poiont particles, are interconnected with homotopy via mini-string -- and mini-string chords are substringular fields.), as well as the flow of the substringular encoder patterns that surround the associated Planck-Related phenomena.      Negative-Norm-States form ghost-anomalies by tracing where substringular phenomena have distributed per each prior instanton.  Positive-Norm-States undo ghost-anomalies by scattering the prior mentioned traces on account of the reverse-holomorphic flow that positive-norm-states undergo to undo these mentioned ghost anomalies over a relatively small sequential series of instantons.  Normally, a substringular phenomena bears a ghost trace of where it was in a prior iteration.  In a relatively small number of instantons later, norm-states that move in the opposite direction as those that form an arbitrary ghost-trace scatter the ghost traces in order to free-up room in the substringular.  Zero-Norm-States help convert one-dimensional superstrings, which are the discrete holonomic structure of the permittivity of plain kinetic energy, into the discrete holonomic structure of the permittivity of electromagnetic energy, which are comprised of certain two-dimensional superstrings.  This is true in the case of the Fujikawa Coupling. The Fujikawa Coupling involves the interaction of zero-norm-states that pull at an apex in-between two chords of mini-string that tug in an abelian manner with the mentioned one-dimensional superstring, while yet moving in the direction of the propgagtion of an arbitrary one-dimensional superstring that is closing to form the said two-dimensional superstring by harnessing the two ends of an open-string in such a way so that the closing of the mentioned open-string  is in the opposite direction of its propagation.  This is even though the Fourier Translation of the Fujikawa Coupling as a unit is in the general direction of the forming of the soon to be bosonic string portion of a photon.  As a coralary, zero-norm-states often help convert the two-dimensional superstrings' holonomic structure of permittivity into the holonomic structure of permittivity of one-dimensional superstrings when a photon is converted into plain kinetic energy via a forward-holomorphic wave-tug that opens a closed string in a hermitian manner via the inverse of the Greene Function.  Negative-Norm-States harmonize stringular propagations.  --  These show physical evidence of discrete Hamiltonian holonomic structure.  Positive-Norm-States add anharmonics to substringular propagators.  --  These scatter evidence of discrete Hamiltonican holonomic structure.                         

Part Four of the Eigth Session of Course Nine

The added dimensionality of two-dimensional superstrings causes them to have not only two-dimensional discrepencies, yet also to have three-dimensional discrepencies.  So, one-dimensional superstrings have discrepencies that exist on the relative reverse-norm-to-norm-to-holomorphic side of the Laplacian settings that these exist in at their topological center.  (This center being closer to the relative norm-to-holomorphic Laplacian end of each individual superstring that is to be considered.)  Two-Dimensional superstrings have discrepencies that are both to the relative holomorphic side of the general topology of the mentioned superstrings per each Laplacian setting at the relative 90 degree mark, while these described discrepencies per each Laplacian setting are simultaneously placed in the relative norm-to-holomorphic position at the relative 90 degree mark of the same arbitrary two-dimensional superstring.  At the relative 270 degree mark of any given two-dimensional superstring, the discrepency from the hermitian Laplacian topological flow of the mentioned superstring exists in the reverse-holomorphic position, while the described discrepency per each Laplacian setting are    simultaneously placed in the relative norm-to-reverse-holomorphic position.
Again, one-dimensional superstrings that act as discrete units of energy permittivity bear one discrepency, while two-dimensional superstrings that act as discrete units of energy permittivity bear two discrepencies.
What I mean by discrepencies are seperations from the Laplacian hermitian topological flow of the delineation of the first-ordered point particles that comprise one and two-dimensional superstrings.
Substringular field in the form of mini-string still interconnects the described discrepencies with the rest of the  correlative superstrings during each Laplacian setting that form the basis of the conformal dimension of each superstring that exists in some sort of hermtian topological delineation during each  BRST duration that comprises the majority of the duration of each instanton that happens in the course of substringular iteration.  The added entropy that happens to the mentioned two-dimensional superstrings causes these to form more dilatons when these mentioned superstrings are propagated through space.  This configuration of discrepencies (partitions) causes these to "flap" a little bit more than one-dimensional supestrings when these are propagated through space.  The faster the mentioned two-dimensional superstrings travel transversally per iteration at under light-speed when the light-cone-gauge topology of the described two-dimensional superstrings is Kaluza-Klein,  (Kaluza-Klein meaning to bear an abelian light-cone-gauge topology.) the more that the associated two-dimensional superstrings tend to "flap."  As the Planck-Related phenomena that are associated with two-dimensional superstrings that are of a Kaluza-Klein light-cone-gauge topology flap, the corresponding two-dimensional superstrings flap in synchronicity with the prior mentioned Planck-Related phenomena.  Yet, Yang-Mills bosonic superstrings are often electromagnetic in nature, which causes these to travel at light-speed when in a vacuum, which decreases the inefficiency of the prior mentioned "flapping."  This is because the added wave holonomic condition that exists here provides a homostasis that tends to support the holonomic stability of the superstrings here due to an increase in the fractal modulae of the said superstring on account of the mentioned physical counterbalances that thus happen here.  One-Dimensional superstrings tend to orbit back-and-forth upon their axes as these are propagated through space.  I will continue with the last part of this session later.  Until then, God Bless You in the name of Yahweh, and I hope for only positive things for all of the readers who read my blog posts.               
Sincerely,
Sam Roach.             

More About The Dangers Of The Hadron Colliding Experiment

Hello, my name is Sam Roach. I don't get too much into philosophy. I get into the mechanics of the substringular. E(6)XE(6) superstrings that are adjacent are to spin assymetrically. E(8)XE(8) superstrings that are adjacent are to spin assymetrically. E(6)XE(6) superstrings, if pulled away from their corresponding light-cone-gauge eigenstates, would work to make -- at least -- a fissure in the Rarita Structure. E(8)XE(8) superstrings, if pulled away from their corresponding orbifolds and orbifold eigensets, would work to make -- at least -- a fissure in the homotopy of adjacent orbifold-like structures. Endangering a local homotopy can easily form a domino effect that could ruin space-time-fabric.                 


Please end the Hadron Colliding Experiment.
                                                                                                                        
Sincerely,

Sam.