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Both DIONS
and TRIONS
may demonstraate forces-at-a-distance, inclusive of nuclear forces of repulsion
and attraction, electrostatic forces of repulsion and attraction, magnetic
forces of repulsion and attraction and the gravitational force which seems
to tug in only one direction, that is until the distance between mass centers
decreases to around 10-15meters.
The makeup and occurrence
of these field objects within groups, as well as simple waves, is affected
by the presence of compatible and incompatible field objects: those
objects which seldom interact or interact without destruction and those
which mutually annihilate each other at every opportunity.
At the onset of
the establishment of any group, any one of the six possible layers will
play a role in governing this makeup. Though there is
no preset orientation of layers within any finite region of the field,
once established though, the layers remain either parallel or orthogonal
to each other, as long as there are a significant number of field objects
supporting their arrangement. Normally, within any finite region
of the Random Field, there is no existence of layers; layers being
purely functional. This means that the field itself, and photons,
are colorless.
As a matter
of convention, the first layer to be identified is the red
layer, its normal the x-axis. The next layer is the green layer,
its normal the y-axis. The third layer is the blue layer,
its normal is the z-axis.
The three
axes are equivalent to the three axes of a left-hand Cartesian coordinate
system.
You will need
to commit to memory this order: x-y-z to R-G-B. The remaining
layers, also corresponding to x-y-z are the subtractive
opposites: cyan opposite red, magenta opposite green and yellow opposite
blue.
The R-G-B group is further delineated by polar impulse of ISSs as designated
by the left-hand rule: the thumb showing the direction of the polar
impulse as directed along the axis of spin of the ISS, this direction,
by convention, being designated as NORTH.
The direction of the four fingers represents the direction of orbit of
the simple wave comprising the ISS. Of course, we have already gone
through this, but it doesn't hurt to repeat it, especially since now, because
we will be using it.
If the NORTH
axis points in the positive direction of these axes, then the layer which
this object normally occupies is a primary layer belonging to the group
R-G-B, and the spiral object (aka: toroid) itself (ISS or OSS) is considered
positive.
If the NORTH
axis points in the negative direction of these axes, then the layer which
this object normally occupies is a secondary layer belonging to the group
C-M-Y, and the spiral object itself (ISS or OSS) is considered negative.
Presumably,
the formation of a DION
from spiral configurations may more readily occur than the formation of
a TRION,
simply because only two spiral configurations are required, rather than
three.
It also seems
that spiral configurations with similar shell radii will most likely combine
than those with dissimilar radii. This means that an ISS will more
likely combine with another ISS, than an OSS, and that an OSS will more
likely combine with another OSS, than an ISS.
Such being
the case, two ISSs may come together with axes orthogonal, forming a DION.
As such, given one of its constituent ISS originates in the red layer,
its other ISS may come from the green or blue layers, or from the opposite
magenta or yellow layers.
It cannot come from the cyan layer, because the normal to the cyan layer
is parallel to the normal of the red layer.
On the other
hand, the combining of a red ISS and a cyan ISS, would generate a dual-wave
radial configuration (object) whose polar axis parallels the X-axis of
the QCD
frame of reference. If this was repeated again, combining opposite
Z-axis ISSs together, and then combining both the X and Z-axis dual-wave
radials without change of orientation, we would then have an X-Z neutral
DION,
as pictured right.
If again we combine a Y-axis dual-wave radial with the X-Z neutral DION,
we end up with an X-Y-Z neutral TRION
pictured left.
All dual-wave
radials comprising the neutral TRION
are momentarily stable, though each eventually succumbs to dissociation
of their own two waves from each other and from the orbital center, all
of which is directly dependent on their respective orbital radii.
This is both predictable and a matter of time. It can only be assumed
that once dissociation commences, it rapidly affects the entire TRION,
causing its breakup to form two new TRIONS:
an ISS TRION
and an OSS TRION.
ISS TRIONS
carry a charge and show inertial characteristics. OSS TRIONS
also carry a charge, but do not demonstrate inertial characteristics.
Both are stable and do not decay.
During dissociation,
paired waves, those belonging to the one plane of the dual-wave radial,
take wild orbital swings, one driving inward and the other driving outward,
and then reversing; the outermost wave striking an inside orbit and
the innermost wave striking an outward orbit. This oscillation between
them continues until dissociation completes itself, leaving these counter
rotating waves at dissimilar orbital radii.
Considering
all three X-Y-Z dual-wave radials, now dissociated to the extent that their
counter rotating waves no longer have the same period, the three waves
with short radii will begin to wind up into a set of orthogonal spirals
to the interior and the three waves with the larger orbits will do the
same.
If these
two groups of three orthogonal spirals can maintain coherency and yet dissociate
from each other, two new TRIONS
will be generated.
If the three
waves with the shorter radii all belong to a common QCD
set, either having the colors RGB
or CMY,
the outermost set thus being the opposite (secondary QCD),
the two new TRIONS
will either be an electron-proton couple or an antiproton positron couple.
Upon completion
of dissociation, the objects of the resultant couple, having opposite charges
(opposite spirals) and magnetic poles, NORTH
to SOUTH
facing, will constantly attract each other in six ways: three radial
attractions and three polar attractions.
The end result
of this is that two new TRIONS.
In this hypothesis,
very small field waves are geometrically not disallowed, these prospective
waves though unable to flourish pragmatically in a field of a given finite
density. As pointed out before, this threshold of success or failure
is approximately 3h, where h is the reciprocal of the field density.
Not covered
by discussion, though mentioned, one can expect exceptionally high field
densities in regions of the field which are very active in particle and
energy activity. Accordingly, in such places, such as the sun, very
small waves can be expected to flourish in very high numbers.
The required
spirals for a neutral TRION
dual-wave radial come from adjacent X-Y-Z layers.
If any spiral
is able to cross into an adjacent layer, normally repulsed by polar coupling,
the polar coupling will subside as radial attractive coupling prevails,
pulling this spiral, say a cyan spiral, into concurrence to a red spiral;
their respective waves seeking a common orbital plane. In this state,
the spirals are momentarily confined to this orbital plane as counter rotating
waves, which quickly unwind the spiral fields associated and once maintained
by each spiral, into a purely radial field without any spiraling.
Once achieving this new state, the standing wave condition abates, and
each wave is able to migrate outward with each orbital passage, slowly
enlarging their respective orbital radii until dissociation occurs.
This process
is driven by increasing saturation
of layers forcing more and more spirals to cross over; setting up
these conditions so that they occur at an ever increasing rate.
As this process
increases in its frequency of occurrence, for all neutral X-Y-Z DIONS,
TRIONS,
in this case neutral TRIONS,
will be produced by an ever increasing rate, until equilibrium in their
numbers is presumably reached.
This is an
irreversible tendency, that once orthogonal X-Y-Z neutral DIONS
convene in proximity, they will be inexorably drawn
together forming neutral TRIONS.
At this stage,
we have a neutron which has already commenced its decay sequence.
This sequence, previously outlined should yield two opposite charge R-G-B
TRIONS
as illustrated following and thoroughly discussed here.
Principal
dissociation stages include outward migrating orbits of dual waves simultaneously
along the X-Y-Z axes until radial dissociation is reached, polar dissociation
of the two new opposite charged TRIONS,
radial attraction of opposite charged X-Y-Z planes of each TRION
establishing a TRION
couple and the persistent motion of the OSS TRION
forcing it to orbit the ISS TRION
of this couple.

coming from the electron
itself, since they are moving with it.
n exceptionally close distance
(10-15 meters), the immutable geometric impulse reverses itself,
disallowing the electron from approaching any further, binding it in orbit.
Rather than
a smooth orbit, the electron careens about a nucleus of three orthogonal
ISSs which produce an uneven and lumpy field for it to move, as well perhaps
the opportunity for it to escape.
If indeed
polar
separation occurs first, both proton and electron will become free particles
wandering about the field and mingling among the six layers, ready to join
with what ever comes along or is pushed their way.