1
Quantum Symmetry
Page Index
2 Quantized Symmetry
for Topological Energy
Particle Modeling
Frequency Pulsation
2 Quantized Symmetry for
Topological Energy Particle
Modeling
The quark-string model for force points as fundamental particles of matter was unified with the
expanded Schrodinger equation for one atom with quantum symmetry numbers as a variableto build a
valid definition within the particle in a box argument's terms. Mapping that for topological clarity led to
the inclusion of supersymmetry as a key feature, and since symmetry is a force it must be quantized.
Symmetry is taken to be a field force consisting of quarks of the next smaller dimension of quanta, a
size of about 10 ^-56 J. That scale is named the D5. Quantum symmetry is uncanny, giving a perfectly quantized,
symmetric design to the Ge atom.
Since symmetrons are D5 quarks They are identical to the D4 ones, at right
find the topological map of the hexon. It's quantum symmetry numbers are {*3,*4,*6},
while it's six open faces act by organizing hexasymmetry among particles within it's
matrix-field. Mineral quartz crystals are bonded by hexasymmetrons as a force field.
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Next, by that definition we need a variable to represent the quantum symmetry numbers in our
atomic topofunc and all of the relative quantum particle functions for the
complete set of energy particles, including the electron topofunc. This is the {*n, Sn } variable. A symmetron joule
value exists for each column of the table of relatons and fundamons, with
the energy value stored in it equal to the rels of that column's single relaton.
Hence each successive order of the series differential
expansion of the Schrodinger equation denotes a new plasma stage of
the nucleus, and each advance to a new stage elicits emission of one Q4
equivalent of that symmetron from the nucleons, due to the compressive,
concentric force of the electromagnetation stages which contract the atom
and trigger all of it' electromagnetons to emit all internal, asymmetric energy
as em photons to the enviroinment. By this nucleon excitation the nucleons
spin and emit their successive stages of advancing symmetrons. They form
wells like geysers as they move toward the nuclear surface, as shown at right.
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