The light-cone-gauge field of a first-ordered light-cone-gauge eigenstate bears five links of mini-string when involving one-dimensional superstrings and ten links of mini-string when involving two-dimensional superstrings. With the field of a light-cone-gauge eigenstate that involves a one-dimensional superstring, the five mini-loops consist of two segments of mini-sstring each that are looped around each other. When it comes to the field of a light-cone-gauge eigenstate that involves a two-dimensional superstring, the ten mini-string links are not Gliossi to any mini-string except that of the ten mini-string segments that bind the associated two-dimensioal superstring that is being discussed here with its correlative Fadeev-Popov-Trace. A Fadeev-Popov-Trace is the field trajectory of a superstring. A Fadeev-Popov-Trace is a discrete unit of energy impedance, while a superstirng is a discrete unit of energy permittivity. A superstirng consequently may be viewed of as a field trajectory of a Fadeev-Popov-Trace, yet, in the opposite tense of holomorphicity as the other way around. Light-Cone-Gauge eigenstates may either be abelian in geometric nature, or, these mentioned general types of eigenstates may be non-abelian in geometric nature. An abelian light-cone-gauge eigenstate has a supplemental wave-tug in-between a related arbitrary given superstring and its correlative Fadeev-Popov-Trace. The light-cone-gauge topology of an abelian geometric nature is known of as a Kaluza-Klein topology. Light-Cone-Gauge eigenstates that bear a sinusoidal interconnection between the arbitrary given superstring and its correlative Fadeev-Popov-Trace are said to be non-abelian. A non-abelian light-cone-gauge topology is known of as a Yang-Mills topology.
I will continue with the suspence later! Sincerely, Samuel David Roach.
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