An eigenstate of a fractal of a magnetic state may be viewed of as a discrete unit of the spin-orbital momentum of the composite of any given arbitrary superstring, its correlative counterstring, its correlative Fadeev-Popov-Trace eigenstate, and its correlative first-ordered light-cone-gauge eigenstate -- as may be extrapolated during one respective given arbitrary iteration of group-related instanton -- in which such so-stated physical states may be considered of as working to bear such a so-eluded-to homotopic relationship. The said superstring and its directly corresponding counterstring work primarily as the Hamiltonian operators of one respective given arbitrary unit of discrete substringular angular momentum, and thus, the said superstring and its correlative counterstring act primarily as a fundamental fractal of an electric charge. (Since electric charge is due to the processes of permittivity). This happens, as such a so-stated superstring and its correlative counterstring are pulled along in the substringular -- over a successive series of group-related instantons. The said Fadeev-Popov-Trace eigenstate and its directly corresponding first-ordered light-cone-gauge eigenstate, work primarily as the Hamiltonian operators of one respective given arbitrary unit of discrete substringular spin-orital momentum, and thus, the said Fadeev-Popov-Trace eigenstate and its correlative first-ordered light-cone-gauge act primarily -- as a fundamental fractal of discrete magnetic force. (Since magnetic force is due to the processes of impedance.) -- as such a so-stated Fadeev-Popov-Trace eigenstate and its correlative first-ordered light-cone-gauge eigenstate, are pulled along in the substringular, over a succession of two or more consecutive group-related instantons.
To Be Continued! Sincerely, Sam Roach.
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