Gauge-Fields & Gauge-Ghosts

When a superstring iterates at a specific locus at BRST, its gauge-field (the location of its first-ordered-light-cone-gauge eigenstates) bears an initial locus in space before the associated second-ordered light-cone-gauge eigenstates are plucked by the correlative gauge bosons that are in the general field neighborhood of the appertaining first-ordered-light-cone-gauge eigenstates. When the mentioned light-cone-gauge eigenstates are plucked, the resulting vibrations are dirstributed through appertaining Rarita Structure eigenstates through the Ricci Scalar eigenstates to the gravitinos that are the most directly connected to the associated superstrings. After the Imaginary Exchange of Real Residue during an iteration that does not involve the Kaeler metric, the light-cone-gauge springs holomorphically for forward time moving particles and antiholomorphically for backward time moving particles at the same time to allow for ultimon flow. When the associated superstrings reiterate, the given light-cone-gauge reiterates too -- both of these at a slightly different locus and with a slightly different neighborhood if the superstrings exists in a Noether manner OR these exist in a very different locus and with a very different neighborhood if the superstrings exist in a tachyonic manner. The past light-cone-gauge eigenstates form a set of ghost anomalies, once that these go through ultimon flow, and the interaction with norm states (positive norm states) forms dilatons and dilatinos and/or residual norm states that are recycled under Cassimer Invariance. The differentiating field of a light-cone-gauge eigenstate may form a Gliossi interaction with other of such light-cone-gauge eigenstate fields via a homeomorphic cohomology that is majorized planar Yakawa. This wouldn't appertain to the first-ordered-light-cone-gauge eigenstates themselves forming the cohomology, yet the waves induced by the given light-cone-gauge eigenstates that are multiplicitly proximal that interbind to form a polar slope that has torsional handles on the norm to holomorphic and the norm to antiholomorphic sides of these given fields. This is due to the kinematic differentiation of the light-cone-gauge producing a spherical shell that interacts with an appertaining orbifold to form an orbifold impedance via the spatial relation of second-ordered-light-cone-gauge eigenstates. This impedance, through gravitational interaction and norm Ward Conditions , including the interaction of norm states, allows orbifolds to coalesce into orbifold eigensets without the detriment of an Imaginary supercharge. Such "handles" of field may be looped together via the multiplicitly abelian interconnections that allow orbifolds to form a cohomology to form orbifold eigensets. As an orbifold is transferred via a certain gauge transformation, the "handle" of Yakawa Coupling is split and refabbed after splitting as the associate orbifold is brought elsewhere. Such an orbifold shell, with its multiplicit light-cone-gauge first-ordered states, is "circular" with one-dimensional superstrings and with two-dimensional superstrings. These are torroidal in nature. So, a one-dimensional orbifold shell is as a torroidal disc with spherical shaft-like handles, and a two-dimensional orbifold shell is a torroidal shell with "slab-like" handles.