Session 9 Of Course 12

Fermions are particles that are made up at least in part by one-dimensional superstrings that are attached to Planck-like phenomena.  One and two-dimensional strings iterate every 10^(-43) of a second over the course of each successive duration of group instanton.  One and two-dimensional strings are attached to Planck-like phenomena via light-cone-gauge eigenstates. There is one light-cone-gauge eigenstate that attaches each superstring to its correlative Planck-like phenomenon.  Each light-cone-gauge eigenstate of a one-dimensional superstring is composed of five strand-like segmental links.  The just mentioned links of light-cone-gauge eigenstates of one-dimensional superstrings are -- in general -- twice as thick as the strands of the second-ordered light-cone-gauge eigenstates that work to comprise the first-ordered light-cone-gauge eigenstate of  two-dimensional strings.  One end of the just mentioned strands of a light-cone-gauge eigenstate is attached to the mini-string segments of the angular momentum indices of a Planck-like phenomenon, while the other end of the said strands of the said light-cone-gauge eigenstate is attached to the mini-string segment of the directly corresponding superstring of discrete energy permittivity.  One-dimensional strings may iterate as arcs on occasion.  One-dimensional strings are ideally -- in theory -- relatively straight strands of phenomena that are of the Planck-Length, except for their partitions that exist in at least the central general region of the Poincaire-based field of the just mentioned superstring.  Let's say that at one iteration of group instanton of a one-dimensional superstring, the said superstring is arced on either side of its general topology by a certain measure of Laplacian-based mapping of its scalar amplitude.  In-between the just said iteration of group instanton that directly corresponds to the eluded to scenario, and the directly ensuing iteration of group instanton of the selfsame phenomena, the given arbitrary said one-dimensional superstring fluctuates harmonically in terms of the first-ordered point particles that work to comprise the mentioned superstring.  This eluded to harmonic oscillation, in this case, works to define the condition that even though the relatively separated first-ordered point particles that separate here on account of the activity of the directly associated local eigenstate of Polyakov Action stays in as relatively close proximity as feasible, in spite of the directly related Clifford Expansion that acts as the inverse as to how such superstrings are contracted to our vantage point, except that these said point particles will here wiggle out of place a little bit here in a manner that works to help such first-ordered point particles to converge soon after the general activity of BRST.  This differs from the perspecitive as to if the directly related oscillation was harmonic, in such a manner to where the said convergence of the prior said condition is scrambled when in terms of the order of the physical configuration of the corresponding point particles per kinematic mapping of the eluded to reverse-differentiated condition of the said superstring per sub-Fourier inspection at the extrapolation of each gauge-metric in which such an activity may be mapped as such when this is  considered directly after the given arbitrary BRST conditions.  Whereas, if the said format of oscillation were instead harmonic, the phsyical extrapoltaon of the integration the loci of the directly related first-ordered point particles that work to comprise the said string would bear an even isomorphism as to the mapping of the directly related condition of the said superstring as it goes out of BRST. When the said point particles of the said one-dimensional superstring work to reintegrate back into the condition of acting as a superstring, the corresponding one-dimensional string will here iterate as an arc that will here bear the opposite isomorphic genus of concavity than what it had during the directly prior conditions.  Any single arced one-dimensional superstring that is not about to form a two-dimsional superstring always undergoes this process until it is conditioned to either become a relatively straighter vibrating strand -- besides the one or more partitions that work to define the vibratorial index of the said superstring --, or, until it is conditioned to become a swivel-shaped superstring.  Sincerely, Sam Roach