More About Photon Formation

When a fermionic superstring of an electron has its Campbell indices of its field generation struck, it alters to form a bosonic superstring. As the superstring discussed has its field projection struck, the one-dimensional superstring discussed will torsion initially to allign in the direction that it is to scatter in. In the time or metric between two successive Kaeler metrics, the associated one-dimensional superstring aligns in its direction as its Campbell field indices are struck to allow the reverse holomorphic direction of where the superstring is to scatter to begin the Fujikaws coupling discussed. The holomorphic direction of where the superstring is to scatter is where the light-cone-gauge eigenstate associated is directoralized as a gauge-action. The one-dimensional superstring initially realigns to form the directoralization where it is to scatter, while then scattering outward to form a two-dimensional superstring via the Green function via a Yakawa coupling known as a Fujikawa coupling. This here will involve two immediately successive gauge transformations, which are examples of two successive Gaussian Transformations. The aligning of the associated Campbell projected field of the one-dimensional superstring that will form a two-dimensional superstring will alter the physical norm conditions of a locus of superstrings. This "backgammoning" is what forms a Gaussian transformations here. The difference between a gauge transformation and another Gaussian transformation is that gauge transformations always involve entropy, seeing that Kaluza-Klein topology always involves entropy. If the light-cone-gauge topology is maintained, the Gaussian transformation is not gauge.