Fermion states, 0 electrodynamics

The 0(3) quantum electrodynamic equivalent of the RFR effect has been numerically analyzed by Crowell [17] using the Hamiltonian (327). Numerically, it is possible to consider only a finite number of photon modes, and the difference in energy between these modes is set equal to the difference between the two spin states of the fermion. More complex situations were also analyzed... 

In this section we discuss the nonrelativistic 0(3) b quantum electrodynamics. This discussion covers the basic physics of f/(l) electrodynamics and leads into a discussion of nonrelativistic 0(3)h quantum electrodynamics. This discussion will introduce the quantum picture of the interaction between a fermion and the electromagnetic field with the magnetic field. Here it is demonstrated that the existence of the field implies photon-photon interactions. In nonrelativistic quantum electrodynamics this leads to nonlinear wave equations. Some presentation is given on relativistic quantum electrodynamics and the occurrence of Feynman diagrams that emerge from the B are demonstrated to lead to new subtle corrections. Numerical results with the interaction of a fermion, identical in form to a 2-state atom, with photons in a cavity are discussed. This concludes with a demonstration of the Lamb shift and renormalizability. 

Ultimately, the theory must be consistent with quantum electrodynamics, which reduces in the absence of radiative terms to a time-dependent equation, in which i/ is interpreted as a fermion field operator Y state function field equation of motion is equivalent to simultaneous equations... 

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