389(6): Final Adjustments to Note 389(5)

In this note the complex conjugate spin connections (1) and (2) are given for plane waves and B(3) theory. These are maps of the aether or vacuum. They were computed by co author Horst Eckardt using the equations of conservation of antisymmetry for B(3) theory, nominated for a Nobel prize several times. For plane waves the Lindstrom constraint reduces to Eq. (14). The Lindstrom constraint is the trace antisymmetry law of physics. It is written self consistently with the vector antisymmetry laws of physics, Eqs. (11) to (13). The trace antisymmetry law and scalar antisymmetry law (15) must be solved simultaneously and self consistently. This is achieved by defining A*(total) as in Eqs. (20) to (23). This procedure means that the homogeneous field equations (16) and (17) are obeyed automatically on the ECE2 level in physics. For plane waves the electric field strength E is known so the scalar potential for plane waves can be found from Eq. (24), knowing the spin conenction vector. Then the scalar spin connection can be found from the Lindstrom constraint. This is another map of the vacuum for B(3) theory. Maps of the vacuum exist for any theory of physics on the ECE2 level. Finally the scalar antisymmetry law (26) must always be obeyed. This can always be achieved by using the gauge transformation (27), and by adjsuting the gauge function chi. Antisymmetry conservation is a major discovery in physics, as was B(3). So this note can be used in Section 3 of UFT388 The gauge procedure is new to this note, and can also be used in gravitation on the ECE2 level. This is far in advance of the standard model.

a389thpapernotes6.pdf

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