FTAAN, Session 15

Protons and neutrons exist in a state of conformal invariance when these exist in the nucleus. Protons and neutrons consist of quarks, leptons, and gluons. A proton consists of gluons, two quarks, and one lepton. A quark has a charge of (+2/3). A lepton has a charge of (-1/3). So, a proton has a charge of (+1). A neutron consists of gluons and two leptons and one quark. So, a neutron has a charge of 0. Neutrons are neutral in charge. Neutrinos are also neutral in have. Protons and neutrons both have gluons, and gluons have no charge. Protons and neutrons differentiate in a vibratory kinematism that generally has a harmonic transversal motion that bears a parity and chirality that is even and Real in terms of the relatively stable oscillation of the particles that are relatively stationary when one takes the first-ordered relative motion of these given particles during transient periods of time when the given protons and neutrons are not physically perturbated by an outside force. The particles of the given protons and neutrons at the substringular level differentiate superconformally except for the vibration of the particles, although this superconformal behavior is not as limited to the prior said differentiation as with the gluons when one considers the successive motion of the leptons and quarks. The said superconformal behavior only applies to a situation of first-ordered relative motion, such as the eminent behavior of a gluon, quark, or lepton. Neutrinos have an eminent transversal motion that bears a mass of 10,000 superstrings that are Imaginarily Yau-Exact. Imaginarily Yau-Exact means that the superstrings are hermitian and non-perturbative off of and then on the Real Reimmanian plane after successive iteration. This Imaginarily Yau-Exact condition is conformally invariant in terms of the spin-orbital and radial differentiation of the given one-dimensional superstrings, although these given superstrings eminently are propagated through a transversal kinematism that differentiates directorally in a relatively Snell manner, unless these are electrodynamically, or otherwise physically, perturbated by any given holonome that interacts with its Gaussian eigenbasis. If this eigenbasis is altered in such a way that the Landau-Gisner-Action of the given neutrinos happens the Fischler-Suskind-Mechanism alters the Higgs Action in such a way so as to alter the given Klein relation. The Ricci Scalar will then perturbate to produce a Kaeler/Calabi metric that will alter the state of these neutinos. The prior potential of what was neutrinos will now have a dissapation that may, through the proper electromagnetic reinforcement, form a potential energy for the formation of other neutrinos. Hint: Cause the eletromagnetic reinforcement to have a reverse-perturbative potential so as to be able to create neutrino energy from the Kaeler/Calabi heavy water holomorphism that trapped the neutrinos.