(Reprinted with permission)
Mathematical physicist Tony Bermanseder stated:
Allow me to add my understanding of basic geometric spinproperties.
Zeus is describing an elementary association between quarklepton
constituents, which have significant application and are well
understood in the experimental apparatuses.
Rybo I wish I could draw pictures and the like but I do not have
access to the appropriate software and display agencies.
Let us take two leptons, an electron and a positron, both with
fermionic halfspin (s=1/2 in intrinsic angular momentum quantised as
(1/2).(h/2Pi)=h/(4Pi).
If the spins are aligned or parallel, then the electron and positron
can revolve about each other and form a shortlived system called
ORTHOPOSITRONIUM, decaying in so 10^7 seconds into THREE Photons
(which are spin1 Bosons).
Orthopositronium has a combined BOSONIC SPIN of 1 and because of
Maxwell's Equations a 1spin particlestate cannot decay into TWO
photons, as the spins of 1 and 1 cannot conserve the 1 spin of the
Orthopositronium.
If the spins are antiparallel or opposite, however, exactly this
situation occurs and PARAPOSITRONIUM decays into TWO Photons with
opposite spins, cancelling each other as 11=0 and the spinstate of
Parapositronium.
Parapositronium decays in so 10^10 seconds and is longerlived in
the factor Alpha (1/137) becaiuse this is the interaction
probability between a photon and the matter/antimatter state.
Ok then. This process repeats itself in the 'GluonJets' in the
Standard Model.
The Charmonium (J/PsiMeson) decays into THREE GLUONJETS, each
gluon jet partitioning into quarkhadron/meson particleshowers.
The CharmoniumMeson has of course 1spin and is a high mass form of
Orthopositronium.
This then is the parallel/antiparallel spinresonance background,
where pure energy transforms between radiative (photonic) and
massive eigenstates.
We transfer this into the nucleus, found in the basis of the
nucleons (proton and neutron).
Here then you find very stable Heluium4 arrangements of nucleons as
quark extensions, forming sausageshaped or toroidal shapes (Ikeda
Shapes I have posted this here and can resend it).
Particularly, the quark geometry becomes all spindependent.
u.d.u.d.u.d.u.d.u.d.u.d=[proton][neutron][proton][neutron], the
first upquark closing the circle in linking with the last down
quark.
The importance is the symmetry between the ups and downs.
In stability (the most stable Ikeda shape is the one above), the
middle quark in either proton or neutron spins opposite the adjacent
ones.
So you have ++++....describing the superstability of quark
geometry.
Ampere's Laws and Maxwell's Equations come into it, because this
spinning occurs about a magnetoaxis, defining the spinorientations.
I'll repost the udshyperon decay, for you to see the experimentally
verified nature for this.
Well, I'll do this and then you can ask questions about it.
Tony Bermanseder.
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