Synergetic Lattice Field Theory
CONTENTS
ELECTRON 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: Electron Motion. The figure above shows the motion of an electron through a local, two-dimensional cross-section through the synergetic field. In this figure, the center of motion of the electron is defined by the vector equilibrium that is fully contracted to its octahedral phase.
The animation starts with the octahedrally contracted vector equilibrium on the left side of the screen. The octahedral 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 octahedral contraction is clearly visible compared to the vector equilibria further away that are in their isomorphic phases.
In the animation above and the illustration below the transition from the fully contracted vector equilibrium (octahedron) at the center of the electron 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. The illustration shows only the left-handed, octahedrally contracted set of vector equilibria. The complementary right-handed, cuboctahedrally expanded vector equilibria are omitted for visual clarity.
Figure 2: Electron Motion Still-Frame. This figure shows a still-frame from the animation of the localized, electron deformation of the synergetic field shown in Figure 1 above. The centermost isotropic vector equilibrium in the figure is contracted to its octahedral phase. 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 an electron in the synergetic field. An electron 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.