GUFT, Session 8

The gauge-bosons are larger than normal two-dimensional superstrings. Gauge-Bosons are formed by two one-dimensional superstrings that curl, by the Green function, to form a two-dimensional superstring that has a circumference of two Planck lengths. Gauge-Bosons do not cycle the ultimon during ultimon flow. The formation of gauge-bosons from two one-dimensional superstrings is an example of a Yakawa coupling. Yet, since this Yakawa coupling involves two superstrings that curl to form one superstring, and that it does not involve the curling of just one superstring to form another type of superstring, this type of Yakawa coupling is not a Fujikawa coupling. Besides the gauge-bosons, all other types of two-dimensional superstrings are the result of one one-dimensional superstring curling by the Green function to form one two-dimensional string. In either case, the one-dimensional strings that form a two-dimensional string curl in a hermitian manner that thereby obeys the Green function. As gauge-bosons of a gluon pluck the eigenstates of the given Swinger-Indices, and thus these pluck the second-ordered eigenstates of the light-cone-gauge of the given gluon, the eigenstates of the light-cone-gauge are "played" in a harmonic and an anharmonic manner at the same metric. During this guage-metric, both the Yau-Exact and the Wilson-Gordan actions facilitate the gauge-metric action of the light-cone-gauge- eigenstates to form a harmonic dissonance upon the Schwinger-Indices to form a harmonic-anharmonic plucking of the second-ordered-light-cone-gauge-eigenstates. This is done by the Wilson-Gordan actions and the Yau-Exact actions pushing their metric-gauge upon the gauge-bosons to form a vibration of harmonic dissonance upon the eigenstate of the light-cone-gauge. This subordially forms harmonic dissonance upon the eigenstates of the Schwinger-Indices as enacted upon by the second-ordered-light-cone-gauge eigenstates. The plucking of the light-cone-gauge ALWAYS happens during the core of BRST.