The orbital components of any given light-cone-gauge eigenstate acts as activated reigns that helt to push the said light-cone-gauge eigenstate via the activity of the said respective local reigns. The overall forward momentum of light-cone-gauge eigenstates are equal in terms of the holomorphicity of the action that relates to its corresponding Clifford Expansion, except that the directoral permittivity of the corresponding momenta may vary by the type of superstrings that these light-cone-gauge eigenstates are attached to. Light-Cone-Gauge eigenstates of an angular momentum guides its general transversal directoral permittivity. Light-Cone-Gauge eigenstates attached to any given one or two-dimensional superstrings of what I term of as the "upper" half of the Royal Arc have more of a radial momentum that guides its directoral permittivity on account of the condition that the "upper" half of the Royal Arc appertains to the region in which positive moving time is kinematic per iteration of instanton. Light-Cone-Gauge eigenstates that are attached to any given one or two-dimensional superstrings of the "lower" half of the Royal Arc have more of a sinusoidal push momentum that guides its directoral permittivity on account of the condition that what I term of as the lower half of the Royal Arc appertains to the arena in which backward moving time is kinematic per iteration of instanton. I can only describe so much of the picture of the substringular at once.
I will continue with the suspence later! Sincerley, Samuel David Roach.
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