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FIELD OBJECT INTERACTIONS AND COMBINATIONS

    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.

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