It is gluons that work to help, in the connection of those sub-atomic particles that come together -- in so as to form the nucleons of an atom. Gluons are one genus of a sub-atomic particle -- that acts as the eigenstates of the centralized knotting of the Rarita Structure. There are other genre of sub-atomic particles, that work to help connect other sub-atomic particles -- in so as to help to form other particles, besides those particles that work to form the nuclei of an atom, in general. For instance, there is a different genus of a multiplicit eigenstate of the centralized knotting of the Rarita Structure -- that works in so as to bind the three leptons together, that are needed in so as to work to help form an electron. The main difference that exists in-between a gluon (that helps to bind quarks with leptons) and the genus of a sub-atomic particle that helps to bind three leptons together -- in so as to work to form an electron -- is that the torsioining of a gluon, in so as to work to help to make the charges that are directly associated with the nucleons (a positive charge for a proton, and a neutral charge for a neutron), act in a Fourier-based manner -- in such a way, to where this so-eluded-to activity works to bear individually taken whole spins, over time. Whereas, the torsioning of that multiplicit genus of a particle -- that works to help to make the charge of an electron, acts in a Fourier-based manner -- in such a way, to where this so-eluded-to activity works to bear individually taken fractional spins. Bosons work to bear a whole spin, while fermions work to bear a fractional spin. Likewise, that genus, in general, of an eigenstate of the centralized knotting of the Rarita Structure -- that acts in so as to pull together those sub-atomic particles that work to make the composition of a boson -- works to bear torsional eigenindices, that have an integer-based spin. Thurthermore, that genus, in general, of an eigenstate of the centralized knotting of the Rarita Structure -- that acts, in so as to pull together those sub-atomic particles that work to make the composition of a fermion -- works to bear torsional eigenindices that have a fractional-based spin. This is the general case of two different genre of eigenstates -- that are, in general, of the centralized knotting of the Rarita Structure.
I will continue with the suspense later! To Be Continued! Sincerely, Samuel David Roach.
Showing posts with label fermions. Show all posts
Showing posts with label fermions. Show all posts
Friday, August 26, 2016
A Little Bit Of Added Explaination
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Friday, September 20, 2013
The Last Part Of the Ninth Session Of Course 14
The vibrating energy of nucleons is a form of plain kinetic energy, and, this just mentioned energy is therefore comprised of one-dimensional superstrings, or, in other words, these are comprised of open strings. As an object that contains atoms increases in kinetic energy, the object differentiates kinematically with more one-dimensional open strings, likewise. This is because kinetic energy is comprised of open one-dimensional superstrings of discrete energy permittivity. Mass in electrons is comprised of two-dimensional closed superstrings of discrete energy permittivity. Such a given arbitrary mass here -- in the case of electrons -- bears a negative charge. Mass in protons is comprised of closed two-dimensional superstrings of discrete energy permittivity as well. Yet, the difference between the genus of the mass of an electron and the genus of the mass of a proton is related to the spinning tensors of their respective orbifold that work to form both formats of mass as having an opposite genus of spin-orbital parity. Electrons have a fractional spin, whereas, protons have a whole spin. This is because electrons are fermions and protons are bosons. The phenomena of a proton is comprised of more vibrating hoops and less vibrating strands than the phenomena of electrons, on account of the condition that protons bear more mass and less plain kinetic energy than electrons. This is part of what works to cause protons to act as bosons, while, electrons act as fermions. Neutrons are phenomena that are comprised of one quark and two leptons, giving this a neutral charge. (Neutrons bear no physical charge.) Electrons are considered negatively charged because their energy per charge works to repel more per mass than that of their protonic counterparts. -- This is due to the condition that electrons bear a high transversal energy as compared to that of protons. (The given arbitrary electrons of one given arbitrary atom cycle around a relatively speaking motionless nucleus that vibrates in a locally covariant static manner.) Protons are considered to be positively charged because these attract electrons. -- Proton(s) have a wave-pull/wave-tug that acts upon the delineatory basis of the respective electron(s) of any given arbitrary atom. Energy per charge is voltage. Electric voltage works to repel, because the energy per charge that may be considered here works from the interior of the directly corresponding magnetic field of a given said eigenstate of such electric voltage toward the relative outward bearings of the respective Ward-Caucy bounds of the topological substrate where such a field of voltage exists -- this being at a locally static extrapolation of such a field. This corresponds to the condition that electrons are at the exterior of any given arbitrary neutral atom, in relative positioning, when compared to the corelative nucleons, which are interior to the just mentioned electrons. So, when we come into contact with any mass -- what we tend to detect is electrodynamic phenomena. This is why electrons are considered to be the basis of point-mass.
I will continue with the suspense later! Sincerely, Samuel David Roach.
I will continue with the suspense later! Sincerely, Samuel David Roach.
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Wednesday, March 24, 2010
About On-Shell Mass Structure
A two-dimensional superstring has a three-dimensional field associated with it. When a relatively knit Fourier Transform that is highly Laplacian forms a toroidal structure with an annulus at its central coniaxial, the whole Majorana-Weyl supercharge associated with the operation of the associated superstring’s conformally invariant kinematism is delineated, after the group metric that forms the basically Gliossi-Sherk-Olive field described, at the outer shell general locus of that given M-field that is associated with the described kinematic differentiation of the given two-dimensional superstring’s three-dimensional field. This considers the fact that every superstring, whether it partakes of mass or not, has a mass index. Such an on-shell supercharge as taken thru a Fourier Transform that alters the spin-orbital and angular momentum distribution, delineation, and directoralization of the associated three-dimensional field toroidal structure converts the Yau-Exact indices transport in such a way as to form a discrete unit of mass as to the M-field structure that I have conveyed. This is tantamount to that a spherical shell with a physical charge in its center delineates all of the energy of its charge along the topography of its associated shell. Likewise, the norm state Ward conditions of the annulus of a toroidal 3-D field of a 2-D superstring delineates all of the angular momentum and spin-orbital distribution indices at the outer shell of that given toroidal
3-D structure. Likewise, the “figure-eight” twisted toroidal structure created by certain fermionic superstrings forms the point mass of electrons and neutrinos. This mass of certain fermions is created by this: The norm state conditions when considering the Ward conditions of the annuli of the two relatively Mobius ends of the “figure-eight” described have angular momentum and spin-orbital momentum that transfers their distribution and directoralization indices outward to the outer topology of the given “figure-eight-like” structure. The kinematic differentiation of the Yau-Exact indices of the “figure-eight” structure as a whole causes the given phenomenon to translate, thru the Fourier Transform of the given M-field thru a Minkowski or Hilbert Lagrangian, its mass indices into an integration of Hamiltonian eigenstates that allow the Kaluza-Klein phenomena, as with 3-D fields of 2-D superstrings, to convert and/or maintain as a mass. The abelian geometry of the light-cone-gauge of such Yau-Exact structures causes the E(6)xE(6) gauge-bosons related to form Schwinger indices that keep the M-fields oriented to coalesce their Noether indices into a conformally invariant manner that has to be orientable per general locus in order to translate to a proceeding general locus as long as the mass indices associated are limited. Since any M-field needs a limited Lagrangian distribution in order to delineate its Majorana-Weyl indices over a group metric that is based on a harmonics or anharmonics that may not coincide with a group directoralization of Noether flow unless the associated superstring is unorientable, Kaluza-Klein mass is always under light speed, per iteration, and mass must become Yang-Mills as in a worm-hole or Yang-Mills also, if otherwise tachyonic, which is true when mass bears unorientable yet finely directoralized motion via a Ward polarizable dark matter holomorph. Unorientable superstrings may only be as such temporarily when in a large group even if Reverse-Lorentz-Four-Contracted. Mass may become Yang-Mills and tachyonic if its field delineation is majorized.
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