FTAAN, Session 13

When a superstring is superconformally invariant it is limited in its sway of differentiation. Let us consider the differentiation of the superconformal superstrings of a gluon. The superstrings of a gluon are two-dimensional. These superstrings do not transversally differentiate in a relatively transient period of time, nor do these superstrings kinematically differentiate off of the Real Reimmanian plane after a quantum metric per iteration after the core of BRST has begun in terms of any Kaeler metric outside of the activity that transpires during the instanton-quaternionic-field-impulse that associates here directly with the given gluon. Yet, per iteration the given two-dimensional superstrings differentiate at different radial loci that may be mapped out by considering the Planck associated tendencies that accompany the gauge-metric wave-tug pressures that pull the given superstrings toward or away from the neighborhood of the superstring's field. The two-dimensional superstrings will begin in a polarized to holomorphic position that is pure Gaussian relative to the field of orbifold eigenset differentiation. The given superstrings will then turn counterclockwise one radian relative to the holomorphic position at the next iteration. The given superstrings will then turn clockwise one radian relative to the holomorphic position at the next iteration. The given superstrings will then pull clockwise as before one more radian at the next iteration. The given superstrings will then turn counterclockwise one radian at the next iteration relative to the holomorphic position. The given superstrings will then tip holomorphically one radian in the next iteration. Then, per iteration, the given superstrings will tip antiholomorphically twice one radian at a time per iteration. Then, the given superstring will tip holomorphically one radian at the next iteration This happens after many iterations at the core of BRST. This will happen until the Landau-Gisner action in automated by a change of Gaussian that happens via a physical perturbation to the given gluon.