
doi: 10.1007/bf02745965
We present a general method to diagonalize the hamiltonian of particles of arbitrary spin. In particular we study the eases of spin 0, 1/2, 1 and see that for spin 1/2 our transformation agrees with Foldy’s and obtain the expression for different observables for particles of spin 0 and 1 in the new representation.
quantum theory
quantum theory
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