Grand Unified Field Theory (GUFT), Session 6

Ghosts anomalies are formed whenever superstrings, world-sheets, and/or light-cone-gauge eigenstates kinematically differentiate. So, whenever a superstring, a world-sheet, or a light-cone-gauge-eigenstate moves per iteration, ghost anomalies form. The more conformally invariant a superstring, a world-sheet, and/or a light-cone-gauge eigenstate is, the more readily the corresponding ghost anomalies relating to these are annihilated. When ghost anomalies are annihilated, these are scattered off of the Real Reimmanian plane and are sent to the fabric of space-time initially as dilatons and dilatinos that quantize into gravitons and gravitinos. Once the negative-norm-states are converted into particles of gravity, these form Ricci Scalar eigenstates with superstrings that share a tug on these given superstrings so that the particles of gravity may be able to exert a gravitational pull on substringular phenomena. Since dilatons, dilatinos, gravitons, and gravitinos function off of the Real Reimmanian plane, these do not fully cycle around the ultimon as superstrings, stringular encoders, and light-cone-gauge-eigenstates do. The Wilson-Gordan conditions of the superstrings of gluons are anharmonic, while the Yau-Exact conditions of the superstrings of gluons are harmonic. So, the Schwinger Index of the Wilson-Gordan conditions of the superstrings of gluons forms an anharmonic "tune", while the Schwinger Index of the Yau-Exact conditions of the superstrings of gluons fors a harmonic "tune." Some of the eigenstates of the Schwinger Indices of the Wilson-Gordan conditions of the superstrings of a gluon are harmonic while some of the eigenstates of the Schwinger Indices of the Wilson-Gordan conditions of the superstrings of a gluon are anharmonic, while the eigenstates of the Schwinger Indices of the Yau-Exact conditions of the superstrings of a gluon are all harmonic. Wilson-Gordan conditions are the kinematic mapping of Chern-Simmons conditions, while Yau-Exact conditions are the kinematic mapping of hermitian and non-perturbative conditions. The gauge bosons of Wilson-Gordan eigenstates of transposition are Real and Imaginary, since these involve Real Reimmanian and Njenhuis tensors of oscillation. The gauge bosons of Yau-Exact eigenstates of transpositions are just Real, since these only involve a first-ordered Majorana-Weyl oscillation. The gauge bosons vibrate the light-cone-gauge to form eigenstates of the Schwinger Index that form the Schwinger Index. Superconformal ghosts of the light-cone-gauge are created and annihilated right after these are created. Ghost anomalies are not completely physical in the sense that the vacuum regions in-between norm-states indicate to an extent the prior differentiation of certain substringular phenomena, and also because ghost anomalies of light-cone-gauge eigenstates do not get plucked by gauge bosons. Yet, if ghost anomalies were not actually real, there would be no gravity.