Relatively Dense Centralized Knotting

The strong force is multiplict at a locus, at which there is an eigenstate of the centralized knotting of the Rarita Structure.  Gravitational waves tend to move outward and perpendicular to the transversal medium that these are here to be moving through, over time.  The strong force is that force that works to inter-bind those subatomic particles together, in so as to work to bring phenomenology together -- such as that force that works to bring quarks and/or leptons together in so as to form protons, neutrons, and electrons.  A high density of subatomic particles will tend to mean that there will thereby be a high density of atoms.  A relatively high density of atoms eludes to the condition of a relatively high tense of gravity.  The more dense that the delineation of eigenstates of the centralized knotting of the Rarita Structure is, the more that the gravitational force will tend to act upon its surroundings -- in so as to work to push-in such external phenomenology upon itself.  Therefore -- the more dense that the delineation of the strong force is, the more that the gravitational force will tend to act upon its surroundings -- in so as to work to push-in such external phenomenology upon itself.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Session 11 Of Course 4 -- Why Charges Bear Their Correlative Charges

Protons are positively charged particles that have a small amount of mass.  Protons are made up of quarks and leptons.  Electrons are made up of three leptons each.  Protons generally are the simplest particles that exist with a charge that is just as positive as an electron’s charge is negative.  It has a lot more mass than an electron, and its residual energy discharge does not form light.  Electrons tend to move faster than protons, and electrons spin a lot more antisymmetrically than protons.  Electrons each have a fractional spin, while protons each have a whole spin.  A particle with a negative charge will have the opposite spin holomorphicty than an adjacent  particle with a positive charge.  The J is related to the symmetrism of particles, for the reason that J involves the spin-orbital-interactions of particles.  As stated, J is also related to the electric field of a given particle, since, J is related to the angular momentum of a given particle.  Angular momentum is related to spin-orbital-interaction, since the directoral impetus is influenced by the way something spins and orbits.  (The way something goes around influences the direction that it incorporates and the object’s drive in that direction.)  The electric field is that field that is most influenced by its charge.  Since electrons that are adjacent spin antisymmetrically in an atom, and antisymmetric is negative of symmetry, and this symmetrism is influenced by J and thus the charge of an electron, and the holomorphism of the orbit of an electron’s transversal motion is antiholomorphic relative  to the directoralization of the given electron’s path around the nucleus of an atom, the charge of an electron is  negative.  Since protons’ spin in an atom tends to be more symmetric, and the orbital vibrations of protons is holomorphic relative to the general Laplacian setting of an atom, a proton has a positive charge.  Electrons spin antisymmetrically in an atom because of their fractional spin, high velocity, and also because of the dynamics of their fields.  The electric fields of electrons tend to work on the world more than the electric fields of protons.  Remember how light is the result of the recycling of differential geometries?  Remember how the residual discharge of electrons is light?  Electrons do this because these are a point mass of charge versus the mass that appertains to protons and neutrons.  Well, this is why electrons have more dynamic fields that protons.  These electrons thus need to be geometrically arranged so as not to interfere with where these are at.  Electrons, to exist in a spot, have to be in their own spot.  Since their fields are more dynamic, they must spin antisymmetrically to adjacent electrons of the same atom or else these will collide fieldwise.  This description of  an electric field would also help to describe the magnetic field, since magnetic fields curl around electric fields.  If  two adjacent electrons of the same atom were to be perturbated to attempt these  to spin symmetrically, the electrons, instead, would find a new localization, since two things cannot occupy the same spot at the same time.  The field dynamics of subatomic particle is influenced by the velocities and directoralizations of these selfsame particles.  The velocity of a particle influences the field associated with it.  Thank you for enjoying this session.  Have a great day!  I will continue with the suspense later!  To Be Continued! Sam Roach.

As To Phenotypical And Recessive Bonding Cites

  Think of the general condition of both phenotypical and recessive genes, at the level of the nuclei of living cells.  Now, think of such a general condition -- as a fractal that is to here be taken at the sub-atomic level.  Whenever a quark works to bond to another sub-atomic particle -- the bonding cite is always on the quark -- at the gluon of the respective quark.  So, whenever a quark is to bond to another sub-atomic particle -- the bonding cite of the quark, which is at the gluon of the said quark -- is of a phenotypical nature.  So, whenever one or more leptons are to bond to one or more quarks -- the bonding cite that is of such a said set of letpons, is always to tend to be of a recessive nature.  Yet, when two or more leptons bond to one another -- the bonding cites of the said two or more leptons, instead of being of a recessive nature, are to here be of a phenotypical nature. That's all for now!
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Stuff About The Gell-Namn-Najshima Relations

Those sets of boundary-based conditions of the multiplicit acting quarks -- when one discerns the covariance of their so-eluded-to parity-based interactions -- that work to establish the kinematic interplay of their Ward-Caucy bounds, as taken over the multiplicit Sterling-based approximations of their sequential series of iterations, that is of their directly corresponding group instantons, -- that work to form that energy that such quarks function in, in so as to operate as such a partial of any directly related subatomic source of physical entity over time, -- is the concept of as to what may here be termed of as the Gell-Namn-Najshima relations that exist in the substringular.
 I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Gell-Mann-Najshima-Relations

Those sets of boundary-based conditions of multiplicitly acting quarks -- when one discerns the covariance of their so-eluded-to parity-based interactions -- that work to establish the kinematic interplay of their Ward-Caucy-bounds, as taken over the multiplicit Sterlilng-based approximations of their sequential series of iterations of directly assoicated group instantons, that work to form that energy that such quarks function in, in so as to operate as such a partial of any directly related subatomic source of physical entity over time, is what works to define the existence of Gell-Mann-Najshima-Relations.

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.

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."