About the Field Transition During a Fujikawa Coupling

When an electron drops an energy level, a fermionic string of the given electron's plain energy bends heermitianly as the associated one-dimensional superstring is pulled out of the general orbit of the affiliated electron to form a bosonic superstring which, in this case, ks a photon. The hermitian bending or curling of this one-dimensional superstring upon itself to form a two-dimensional superstring that is here a photon is known as a Fujikawa coupling. A Fujikawa coupling is an example of a Yakawa coupling. A Yakawa coupling is the touch, rub, or curl of one substringular phenomena upon another. Such substringular phenomena may be superstrings, Fock fields, Real Reimmanian fields, or gauge-actions. Every superstring has a field associated with it. Such a field bears a tense of spin-orbital momentum and a tense of angular momentum associated with it. A one-dimensional superstring has a thin disclike field associated with it, while a two-dimensional superstring's field has a torroidal shape with a pin-prick hole as its annulus associated with it. The spin-orbital attribute of a one-dimensional superstring bears an unpropagated Majorana-Weyl magnetism unless this magnetism is kinematically driven by a multiplicit Real Reimmanian tensor and/or unless there is a Njenhuis tensor that is associated with the magnetic pretense of the associated one-dimensional superstring's direct field. A one-dimensional field also bears a charge (supercharge) that is associated with its angular momentum. As anything physical has a drive in a direction, all physical phenomena bears an angular momentum. The metric-gauge of a superstring gives that superstring a drive in the direction that its Noether or tachyonic field operators are directoralized in. A two-dimensional superstring also has a spin-orbital momentum and an angular momentum associated with it. The spin-orbital momentum of the given two-dimensional superstring creates a tense of Majorana-Weys magnetism that is able to propagate, even when it (the affiliated two-dimensional superstring) is only unitarily kinematic. A two-dimensional superstring may also delineate a Majorana-Weyl covariant magnetic field when its kinematic field operators are multiplicitly directoralized. As before, a two-dimensional superstring also has a drive in a direction, which is its angular momentum. So, as a one-dimensional superstring bends topologically along the normalcy to its surface to form a two-dimensional superstring hermitianly via the Green function, the field of the one-dimensional superstring likewise bends initially while its edges curved cusps of this field are torsioned outward via the spin-tendency of its metric-gauge to sew the field fabric into a cylindrical shape that involves a relatively thin Neumman-Ward external boundary with a relatively large annulus. This initially happens as the Fujikawa coupling is underway. Once the Fujikawa coupling has finished and the superstring and its field is about to be quantized with other photons that have a completed field, the prior field integration will internally network via external mini-string or external substringular field through the holomorphicity of the prior external topology of the forming photon to form a now torroidal field that is of a two-dimensional superstring, having a majorized plane of holonomic topology that has a pin-prick annulus at its center. Once the newly formed photon is fully quantized, it becomes a group propagatorial eigenoperator named a beam of electromagnetic energy. When a photon is formed that way, it becomes a discrete unit of infrared energy