Take the relativistic solutions ∣ψ(1)⟩ and ∣ψ(2)⟩ of (4-20) for the Dirac equation in the non-relativistic limit, i.e., with v≪1 (c=1 in natural units), and show that they reduce to approximately (1,0,0,0)Te−ipx and (0,1,0,0)Te−ipx. Do these look remarkably like the wave functions of a spin 21 particle you encountered in NRQM, i.e., spin up state e−ipx(1,0)T and spin down state e−ipx(0,1)T?
Operate on each of the two low speed 4-spinor states you found with the 4D spin operator Σ3 of (4-39). Now, operate on each of the two NRQM 2-spinor states above for up and down spin with 21ℏσ3. Do you get the same spin eigenstates and eigenvalues? Does the low speed RQM case for C type (i.e., having spinors ur) particles parallel that of NRQM?