Though initially ignored, well within the constraint of this study, is the notion of field influence, very much in keeping with Einstein's conceived mass distortion of the field, such much so thought Einstein, that a sturdy retooling of zero space appeared to be essential, thus the introduction to the rule that ponderable masses provide or at least cause, by means of their presence only, the deflection of the mile markers of time and space.  Here's how it works.
    The Random Field is a deductive concept with the inductive artifacts of simple waves cascading everywhere within it from every direction, each able to result in the formation of inside-shelled spirals.
    The wave may normally be thought of as a uniform distribution of motion, when such motion coincides to a surface.  In the absence of coincidence, such motion is unknown observationally.
    At the very center of the wave, this motion is maximum, uniformly diminishing at its edges, thus marking the perimeter of the wave, which may be thought of as circular, or nearly circular, in which case, the wave diameter would be the diameter of this circle, roughly speaking.
    The maximum speed of this wave is thought to approach the speed of light c, where such a maximum occurs randomly in nature;  following a standard distribution bell-curve whose shape most likely follows the historical observation in the measurement of the speed of light by numerous researchers for the last several centuries.

    When such motion manifest coincidently to a surface, its appraoch, before impinging with that surface, may come from any angle, but, once associated with that surface, is motion is deemed properly perpendicualr to that surface;  longitudinal directions along the surface being meaningless.
    In this accord, under different conditions of the field, in terms of its general surface orientation, will cause the wave to follow specific paths, such that in a field of purely random surfaces orintation, the wave will follow a zig-zagged path, appearing straight (rectilinear) to the observer, macroscopically.

    In a radial field, the wave will follow a spiral path.

    Since each wave disturbs the field within a nearly circular region following a nearly circular orbit, regions of the field experiencing the greater displacement of surfaces describe a donut shape.  The resulting configuration is stable, and is called a toroid.
    As with any spiral configuration, two types of long-range impulses are possible, one being a net axial impulse causing same directed toroids to attract along their axes and opposite directed toroids to repel, and the other being a net radial impulse causing same directed toroids to attract along a common or nearly common plane their axis and opposite directed toroids to repel along a common or nearly common plane their axis.
    For a moment, let us remind ourselves what a simple wave looks like:
      It is of course, in its most rudimentary form, as purely an abstraction, drawn on a sheet of papyrus of only two dimensions, where somehow, as if by magic, we see three dimensions;  a sort of mound built up by the change in position of a flexible surface because of the presence of motion (a relative change of curvature at adjacent locations), the motion itself somehow smoothly deployed upon this surface.
    Here is another illustration showing the microscopic zig-zag motion of a wave travelling through the field, though macroscopically appearing as rectilinear motion as a photon.

    In this illustration, the wave energy is frozen as it is ready to leave the tenth surface (surface with vector of motion a distribution of wave motion shown)
    The entire distance across this illustration (eleven somewhat parallel surfaces), whereupon the wave is able to travel orthogonally from surface to surface without loss of energy, despite its changing direction.  This distance is somewhere in the neigborhood of 10^-35  centimeters. [READ]
    In this next illustration, we see the entrance of this wave into a finite region of the field, where, dependent upon the angles of the surfaces encountered, the wave may continue straight, or turn left or right, leading to the potential of field wrapping by that wave itself, in which case an inside shelled-spiral configuration is generated, forming a toroidal shaped quark.

    Just like quarks, inside-shell spirals demonstrate impulses previously discussed, which are akin to charge and gravity.  In this illustration we notice that the polar directions are flipped 180 degrees from each other.
    Both always remain orthogonal to the plane of their activity.
    Though this may be referred to as the subjective plane (as related to the observer), it is as well a physically meaningful region in terms of matter and anti-matter prolification.
    As an example, three pairs of orthogonal planes might occur within a finite three-dimensional Reality, each defined within the scheme of quantum chromodynamic colours;  red, green and blue representative of non-anti-matter origination, and their blue minus counterparts (adjacent parallel planes) representative of anti-matter origination.
    By quantum chromatic rules, the magenta plane as specifically shown in this illustration is the anti-matter plane paired with, and also parallel to the green plane, which is not associated with anti-matter.
    Only quarks arising from photons achieving field wrapping into a standing wave on this magenta plane become anti-quarks, along with those generated on cyan and yellow planes.
    In order to distinguish these two magenta anti-quarks from each other, both obeying the left-hand rule, and neither under natural circumstance able to flip to the other's position, they are said to be positive and negative, respectively.
    Because they are positive and negative, or really of reverse spirals, they will tend to attract, especially when coplanar to each other, and annihilate each other, sending their original simples waves off into separate directions.