Developing a unified model of physics and launching a new generation of technology

www.ccp6.ac.uk/booklets/CCP6-2005_vector_correlations.pdf

On page 9 for example it is described how circularly polarized light pumps the m = – 1/2 ground state of rubidium into the m = 1/2 state. This is a transfer of angular momentum. In the standard model there are only two states of angular momentum, right and left, because of zero photon mass, but in the ECE theory the angular momentum also has a longitudinal component. Polarized atoms can be prepared by pulsed laser preparation. Google literature searching is now as good as any big library, so using this method I found that the inverse Faraday effect and the B(3) field have been observed on the sub femtosecond level in a magnetic liquid and reported by a group from China. So it is quite easy to see how B(3) and angular momentum is at work in photodissociation processes, but it is much more difficult to achieve what Kurata has demonstrated experimentally and industrially. The inverse Faraday effect is routine by now.

omega / c is not equal to kappa.

In other words spacetime is a dielectric with loss and permittivity, explaining the origin of the cosmological shift without Big Bang (UFT 49 and 118). For a massless particle:

omega / c = kappa

and the generally covariant d’Alembert equation is the result. In the received opinion of relativity, due to Einstein and others, it can be seen from eq. (5) that the mass m sub 0 is always the same, so R is always that of the free particle:

R = (m sub 0 c / h bar) squared.

However, keeping m sub 0 constant results in disaster for particle physics, as shown in UFT 158 ff and UFT 171. One can now challenge with confidence the very idea of elementary particles, and in fact it is well known that in relativity, there are no particles, there is only geometry and a scaling factor called “mass”, m sub 0. In covariant mass theory the scaling factor is dispensed with, so mass itself becomes part of geometry. Everything in physics becomes geometry, as required by the philosophy of relativity.

a180thpapernotes2.pdf

R = (mc / h bar) squared

so R can also be found from metrical methods.

1) In Eq. (19), replace minus by plus before (epsilon – V) / (2 m c squared).
2) In Eq. (30) the first term is plus and second term minus.

These slips do not affect the final result (41). The mass term is given by some authors and not by others (e.g. Ryder does not give it, and he omits the spin orbit and Darwin terms). It comes from the non-relativistic approximation of kinetic energy given in eq. (22), i.e. epsilon about p squared / (2m). This approximate epsilon is then put back in the third RHS term of eq. (21) to give:

sigma dot p p squared sigma dot p phi / (8 m cubed c squared) = p fourth / (8 m cubed c squared)

with p = – i h bar del.