The light-cone-gauge field of a first-ordered-light-cone-gauge eigenstate bears five links of mini-string when such a phenomena is involving one-dimensional superstrings, and, a first-ordered-light-cone-gauge eigenstate that corresponds to the topological Laplacian mapping of a two-dimensional superstring bears ten links of mini-string. 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-string that are both looped around each other. When it comes to the field of a light-cone-gauge eigenstate that involves a two-dimensioanl superstring, the ten mini-string links are not homotopically Gliossi to any mini-string except that of the ten mini-string segments that bind such a given arbitrarily associated two-dimensional superstring 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 superstring is a discrete unit of energy permittivity. A superstring, consequently, may be viewed of as a field trajectory of a Fadeev-Popov-Trace, yet in the opposite tense of holomorphicity. Such a Laplacan mapping of the described field trajection directoralization is based on the same concept, except that here, the mapping bears the opposite chirality. Light-Cone-Gauge eigenstates may either be abelian in nature, or, these may be non-abelian in nature. An abelian light-cone-gauge eigenstate has a supplemental wave-tug in-between a given arbitrary superstring and its correlative Fadeev-Popov-Trace. The light-cone-gauge topology of an abelian nature is known of a Kaluza-Klein topology. Light-Cone-Gauge eigenstates that bear a sinusoidal interconnection between the 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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