4) The spin-orbital Hamiltonian-based pulse of a given arbitrary superstring -- when coupled with the cross-sectional torque of the topological holonomic substrate of the directly corresponding Fadeev-Popov-Trace -- works to produce the spin-orbital momentum of the directly corresponding light-cone-gauge eigenstate.
5) For an abelian light-cone-gauge topological holonomic substrate, the just eluded to second-ordered light-cone-gauge eigenstates twist at the locus that is Poincaire to the specific delineations where the mini-strand segmental links that comprise the said second-ordered light-cone-gauge eigenstates are at. This is just as the topological substrate of such eigenstates is elongated via the directly related arbitrary given Clifford Expansion that happens during the correlative gauge-metrics of BRST. Meanwhile, gauge-bosons act in such a manner in so that these "pluck" each of such second-ordered eigenstates. For a non-abelian light-cone-gauge topological holonomic substrate, the projection of the corresponding second-ordered light-cone-gauge eigenstates are to be mapped over a sinusoidal standing wave-like trajectory that is fed into the eluded to general locus -- in the form of an expanding topological substrate in the Clifford-based Expansion-like manner that is also true for abelian-based light-cone-gauge eigenstates as well. The difference here is that the Laplacian-based mapping of an abelian light-cone-gauge second-ordered eigenstate is relatively supplementally linear. Again, gauge-bosons act in such a manner in so that these act to pluck the directly associated second-ordered light-cone-gauge eigenstates as the prior happens over the eluded to iterations of the related gauge-metric of a given arbitrary duration of BRST. P.S.: BRST comprises most of group instanton.
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