The Fourteenth Session of Course 13 On Stringular Transformations, Part one

One and two-dimensional superstrings may both have a swivel shape at various different times.  For a one-dimensional superstring, such a swivel shape is like the basic vibrating strand of an open string, except that the said string curves in a sinusoidal manner into a general format of a general condition of a curved standing wave at the respective iterations of instanton -- in which such superstrings are topologically delineated under the general condition of being shaped in a swivel-like manner.  For a two-dimensional superstring of discrete energy permittivity, such a swivel-based shape of a vibrating hoop of phenomenon is like the basic round shape of a closed string, except that the given arbitrary string here curves in a sinusoidal timeless-based mapping of topology into a general format of a curved standing wave at the respective iterations of instanton in which such superstrings are topologically delineated under the general condition of being shaped in a swivel-like manner.  The counterstrings of a one-dimensional superstring that are swivel-shaped are also curved in a sinusoidal-based manner, except that the said sinusoidal-based curvature of the said counterstring of the mentioned one-dimensional superstring that is swivel-shaped are 90 degrees out of phase with the sinusoidal-based curved standing waves of the said one-dimensional strings that are topologically delineated under the general condition of being shaped in a swivel-like manner.

FTAAN, Session 12

A one-dimensional superstring may be swivel-shaped when it is just Imaginarily Yau-Exact or that one-dimensional superstring may be swivel-shaped when it is tachyonic. A two-dimensional superstring may be swivel-shaped in one and/or two dimensions when it is just Imaginarily Yau-Exact, or when it is tachyonic. A one-dimensional superstring may only be swivel-shaped normal to the holomorphic and antiholomorphic plane. A two-dimensional superstring may be swivel-shaped in the holomorphic or antiholomorphic directions, or these two-dimensional superstrings may be swivel-shaped normal to the radial metric of the topology of the given two-dimensional superstring. A one-dimensional superstring has swivel-shapes that are sequentially normal to the holomorphic plane, then normal to the antiholomorphic plane starting from the bottom of the one-diensional superstring to the top when it is tachyonic. A tachyonic two-dimensional superstring has swivel-shapes that are sequentially holomorphic/antiholomorphic, normal inward to the radial metric of the topology of the given two-dimensional superstring, normal outward to the radial metric of the topology of the given two-dimensional superstring. These sequences are spacial sequences and not time-oriented or multiplicitly substringular metric sequences. With two-dimensional sequences, start at 0 pi and go counterclockwise back to 0 pi. This is taken from a holomorphicly-oriented perspective. When a swiveled superstring is not tachyonic, it may be abelian or non-abelian, depending on the topology of the associated light-cone-gauge eigenstates. Yet, tachyonic swivel-shaped superstrings are always non-abelian.