Student Friendly Introduction to QFT · Problem 19

Vectors: Spin 1 Fields

Physics — QFT · dirac-equation-nonrelativistic-limit

Problem

Take the relativistic solutions ∣ψ(1)⟩|\psi^{(1)}\rangle and ∣ψ(2)⟩|\psi^{(2)}\rangle of (4-20) for the Dirac equation in the non-relativistic limit, i.e., with v≪1v \ll 1 (c=1c = 1 in natural units), and show that they reduce to approximately (1,0,0,0)Te−ipx(1,0,0,0)^T e^{-ipx} and (0,1,0,0)Te−ipx(0,1,0,0)^T e^{-ipx}. Do these look remarkably like the wave functions of a spin 12\frac{1}{2} particle you encountered in NRQM, i.e., spin up state e−ipx(1,0)Te^{-ipx}(1,0)^T and spin down state e−ipx(0,1)Te^{-ipx}(0,1)^T? Operate on each of the two low speed 4-spinor states you found with the 4D spin operator Σ3\Sigma_3 of (4-39). Now, operate on each of the two NRQM 2-spinor states above for up and down spin with 12ℏσ3\frac{1}{2}\hbar\sigma_3. Do you get the same spin eigenstates and eigenvalues? Does the low speed RQM case for CC type (i.e., having spinors uru_r) particles parallel that of NRQM?

Related theory

Browse the problem library