GUFT, Session 11

Electrons have wave-tug. Protons have wave-tug. All physical phenomena have a certain degree of wave-tug upon all other physical phenomena. Even ghost anomalies exhibit a certain degree of wave-tug upon all other physical phenomena, and ghost anomalies are often considered to be non-physical, partially since these are only a memory of superstrings and also partially since ghost anomalies of a light-cone-gauge-eigenstate are not plucked by the gauge-bosons that exist in the region of that given light-cone-gauge-eigenstate. Electrons have a charge, as do protons also. Yet, the charge of electrons is negative while the charge of protons is positive. The reason for this is the holomorphicity of electrons versus the holomorphicity of protons. Electrons have a holomorphic wave-tug basis, while protons have an antiholomorphic wave-tug basis. The impetus of an electron is holomorphic, while its impedance is antiholomorphic relative to a framework that establishes the neucleus of t he atom as its center. Since the neucleus of the atom is its center, the impetus of the electrons is left-tended. The impetus of an electron is the metric-gauge directoralization here. The metric-gauge directoralization taken kinematically is its attraction. Protons have an antiholomorphic impetus directoralization, since these want to move outward toward the electron. The reason for this is that protons are bosonic masses of high mass and direct wave-tug upon electrons. This wave-tug is formed by the parity and chirality of the orbifolds and their correlative superstrings. The protons thus have an antiholomorphic metric-gauge directoralization that is kinematically an antiholomorphic attraction. Thus, electrons have an antiholomorphic impedance and protons have a holomorphic impedance, since impedance is an equal and opposite reaction directed upon impetus. Thus, electrons have a holomorphic permittivity and protons have an antiholomorphic permittivity. Parity refers to the spin symmetry, while chirality refers to the handedness of the orbifolds in terms of the relative Gaussian Jacobian eigenbases of the orbifolds and the protons and electrons as a whole. A Jacobian eigenbasis refers here to a relative differentiation in the Gaussian structure of an orbifold.