Research Notes II, 1949

Rest mass of particle m = ħμ. = energy of particle.

no zero pt. momentum.

We must assume the source for ρ has the same periodicity as the field.

describing the emission & absorption processes.

The Schrödinger equation

All the other representations can be obtained from the one already obtained by unitary ħ and fⁿ:

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If

If t=t, both can be obtained from by the same unitary ħ and [formation?], ∴ If t ≠ t', we cannot do this.

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