Field Theory and Abelian Nature(FTaAN), Session 1

Whenever there is torsional force or the force of the scattering of light, there is a substringular force that happens through a transformation known as a Gaussian Transformation. A Gaussian Transformation is a renormalization of the Jacobian eigenbasis that appertains to the orbifold orphogonation that exists for a specific orbifold or orbifold eigenset. This renormalization is a switch in orphogonation orientation and/or switch in orphogonal perturbation that allows the differentials in the given orbifold eigenbasis to seek new ground on account of one or more Wick operators that kinematically switch the quantity and/or quality of the holomorphic and/or antiholomorphic operators that differentiate within the given orbifold or orbifold eigenset. This group differentiation renews the condition of normalization in the individual orbifolds as well as renewing the condition of normalization in the orbifold eigenset as well as altering the orphogonation orientation of the given orbifold eigenset with the orbifold eigensets that surround it. When a Gaussian Transformation happens, the Hilbert space that surrounds it is perturbated to a new orientation of normalcy that forces the spacial display of the orbifolds to alter the spacial relation of the given superstrings to spontaneously differentiate 10-dimensionally so that the differential geometry of the strings differentiates kinematically to reposition the given Li space from its prior condition of conformal structure. With a gauge transformation, there is light scattering. Light scattering always involves a 26-dimensional reorientation that may be tracked down to 12 dimensions as a majorized Hilbert space. This reorientation involves an added differential in the Fischler-Suskind-Mechanism that pulls the Higgs Action toward the furthered or contracted positioning of the superstring, depending on if the light is initially scattered or if the scattered light is beginniing to requantize. A scattering of light initially pulls the superstrings a little bit holomorphically, while when the scattered light begins to requantize, the superstrings are pulled a little bit antiholomorphically. The reason for this is that a wave-like light-cone-gauge eigenstate that becomes supplemental will be pulled to the relative left, whereas a supplemental light-cone-gauge eigenstate that becomes wave-like will be pulled to the relative right. This is relative to the light-cone-gauge eigenstates based on their being a set of timeless phenomena in one frame. Yet strings spatially differentiate. so, a superstring is not in one exact spot during two consecutive iterations. So, the overall holomorphic transition may be right or left moving in either case although the pull relative to a substringular frame is as I have described it, not to mention the multi-dimensional radial pull that superstrings encounter due to spin-orbital and roll momentum that are described by the differential Hamiltonian metric-gauge wave-tug that accompanies any superstring, since superstrings are always kinematic when these are not eaten up by a black-hole.