389(5): The Spin Cyclic Theorem

This theorem defines the B(3) field as in Eq. (24) through the conjugate product of spin connection plane wave vectors. Symmetry shows that omega(3) = A(3) = 0. The vector antisymmetry equations (32) to (34) are obeyed, and the other two antisymmetry equations (46) and (47) are obeyed by using the procedure on pp. 8 and ff. of the Note. This is the best procedure to adapt in every application because it makes sure that the two antisymmetry equations (46) and (47) are obeyed simultaneously and self consistently. So B(3) theory rigorously conserves antisymmetry, as must all theories of physics. There is also a gravitational and fluid dynamical B(3) field. The ECE School of Thought has become independent of the standard model and is forging ahead with rapid advances.

a389thpapernotes5.pdf

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