The Grand Unified Field Theory (GUFT) by Sam Roach, Session 2

The strong force is the force of gluons in the regions in-between the sub-atomic particles that comprise neutrons and in the regions in-between the sub-atomic particles that comprise protons. These gluons are a strong force because these are superconformal in invariance. Gluons individually have an existence of superconformal invariance in terms of their orbifold eigenset. The individual orbifolds of a gluon are always conformally invariant when these are not perturbated by a nuclear fission, a nuclear fussion, or a radioactive decay. The orbifolds of a gluon differentiate in a condition of Gaussian supersymmetry in that the Landau-Gisner action is less often implemented over a significant substringular period because the gluons are what make the nucleons appear as energy that is in static equilibrium. Since the Landau-Gisner action of gluons is less often implemented in a gluon because gluons are relatively good at maintaining their permittivity because of something that I'll later describe as an Anti-De-Sitter/De Sitter gravitational force, there is less than typical Higgs Action implementation UNLESS a gluon is perturbated. Since the Higgs anomalies associated with a gluon are less often kinematic during static equilibrium, the Fischler-Suskind mechanism is usually in tact in a gluon and is not usually taken out of static equilibrium. Since the Fischler-Suskind mechanism for each given Klein Bottle eigenstate is relatively in tact, the Klein Bottle eigenstates of a gluon are relatively stable and non-commutative. Since these Klein Bottle eigenstates are relatively non-commutative, the corresponding Ricci Scalar eigenstates are in static equilibrium in a gluon. Such a static equilibrium forms a condition of mass-binding stability that causes the protons and neutrons to have a stable mass. Gluons, when these are in the process of keeping nucleons together, tend to keep their permittivity fairly well. So, when gluons, which involve the strong force, are set in place, these do not require a lot of added force to retain their permittivity unless these gluons are perturbated. Yet, as gluons are initially translated thru space to help arrange the leptons and quarks together for their initial binding, this process involves proportionally more permittivity on account of the gluons, and, therefore, this initial process also requires proportionally more Higgs force. The Higgs Action may be thought of as the "force."