435(6): Rules for Quantization in m Space
After experimenting with the notes for UFT435, I decided to adopt the rules (1) and (2) for quantization. They are applied for the free particle in this note, but can be applied to any wavefunction. They result in shifts and splittings given by Eq. (14). These shifts and splittings are due to m space, which can be thought of as the vacuum. So this gives an explanation of the radiative corrections in terms of m(r) functions, getting rid of all the obscurities of quantum electrodynamics. Eq. (14) shows that the Planck quantization is modified by the expectation values of m(r) power half. So the latter is quantized, meaning that the m space is quantized. The problem being considered defines the quantization. The free particle problem is the simplest case. This theory shows that general relativity and quantum mechanics have been unified, because m(r) of general relativity has been quantized. So I intend to base Sections 1 and 2 of UFT435 on this note.