Synergetic Lattice Field Theory
CONTENTS
NEUTRINO MOTION THROUGH THE SYNERGETIC FIELD
In synergetic lattice field theory, elementary particles are not entities external to the field, but are rather localized distortions of the field itself. There is no concept of matter and field, or matter and space. Instead there is just the field of space defined by the synergetic field and localized distortions of the field manifesting as the standard model's elementary particles.
Figure 1: Neutrino Motion Through the Synergetic Field. The figure above shows the motion of a neutrino through a local, two-dimensional cross-section of the synergetic field. In this figure, the center of motion of the neutrino is defined by the vector equilibrium that is in its icosahedral phase (shaded blue).
The animation starts with an icosahedrally contracted vector equilibrium on the left side of the screen. The icosahedral contraction moves from left to right across the field of view. It pauses when it reaches the right side of the figure, and then "bounces" back, traveling back to the left side of the screen. When it reaches the left side, it again pauses. When it pauses on either the right side or left side, the icosahedral contraction is visible (with careful inspection) compared to the vector equilibria further away that are in their isomorphic phases.
Because of the small degree of difference between the vector equilibriums' isomorphic phase and its icosahedral phase, this distinction can be difficult to see at first. In order to assist the visualization of the neutrino's motion, the icosahedrally contracted vector equilibrium associated with the center of the neutrino is shaded blue to highlight its location as the icosahedral pattern of contraction moves across the screen. It can be helpful to look directly at the centermost vector equilibrium and watch it expand and contract as the center of the neutrino moves from left to right and back again.
In the animation above and in the figure below, the transition from the icosahedral phase vector equilibrium at the center of the neutrino to the isomorphic phase vector equilibria at the edges of the figures occur much faster than in nature. In nature, this transition is expected to occur across the span of hundreds or even thousands or more vector equilibria.
Figure 2: Neutrino Motion Still-Frame. This figure shows a still-frame from the animation of the localized, neutrino deformation of the synergetic field shown in Figure 1, above. The centermost vector equilibrium in the figure is in its icosahedral phase (shaded blue). As one moves radially away from this centermost vector equilibrium the surrounding vector equilibria gradually morph into their isomorphic phases. This pattern of deformation spanning multiple vector equilibria defines a neutrino in the synergetic field. A neutrino is nothing other than this local pattern of deformation. It is not a separate entity external to the field but is rather part and parcel of the synergetic field itself.