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Some confusions from some recent lectures; I asked the prof, but I still don't fully understand what is going on. We began with the action (tau is some worldline parameter, dots indicate tau derivatives; they are hard to see):
[tex]S = \int d\tau \; \left\{ \dot x^{\mu} p_{\mu} - \frac12 e(\tau) (p^2 - m^2) + f(\tau) (p_{\mu} \lambda^{\mu} - m) + i \dot \lambda_{\mu} \lambda^{\mu} \right\}[/tex]
Varying this action with respect to the five dynamical variables gives the equations of motion
[tex]\dot p_{\mu} = 0[/tex]
[tex]\dot x^{\mu} - e(\tau) p^{\mu} + f(\tau) \lambda^{\mu} = 0[/tex]
[tex]p^2 - m^2 = 0[/tex]
[tex]f(\tau) p_{\mu} = 0[/tex]
[tex]p_{\mu} \lambda^{\mu} - m = 0[/tex]
Promoting x and p to operators and imposing the standard commutation relations, the first three equations (with f = 0) give the Klein-Gordon equation. This much I understand.
However, to arrive at the Dirac equation, the prof's next step is simply to impose anti-commutation relations on [itex]\lambda^{\mu}[/itex], without any motivation, as far as I can tell. Can anyone clarify the reason for doing this? It seems completely arbitrary.
Also, where do the last two pieces in the Lagrangian come from? The first term serves to link x and p as canonical conjugates, and the second term is a restatement of the mass-shell constraint. But the last two terms don't seem to have any prior justification at all. Are they just thrown in there because they result in the Dirac equation? If so, the entire "derivation" is just a circular argument. If the last two terms are put in because of some more fundamental principle, what would that be?
[tex]S = \int d\tau \; \left\{ \dot x^{\mu} p_{\mu} - \frac12 e(\tau) (p^2 - m^2) + f(\tau) (p_{\mu} \lambda^{\mu} - m) + i \dot \lambda_{\mu} \lambda^{\mu} \right\}[/tex]
Varying this action with respect to the five dynamical variables gives the equations of motion
[tex]\dot p_{\mu} = 0[/tex]
[tex]\dot x^{\mu} - e(\tau) p^{\mu} + f(\tau) \lambda^{\mu} = 0[/tex]
[tex]p^2 - m^2 = 0[/tex]
[tex]f(\tau) p_{\mu} = 0[/tex]
[tex]p_{\mu} \lambda^{\mu} - m = 0[/tex]
Promoting x and p to operators and imposing the standard commutation relations, the first three equations (with f = 0) give the Klein-Gordon equation. This much I understand.
However, to arrive at the Dirac equation, the prof's next step is simply to impose anti-commutation relations on [itex]\lambda^{\mu}[/itex], without any motivation, as far as I can tell. Can anyone clarify the reason for doing this? It seems completely arbitrary.
Also, where do the last two pieces in the Lagrangian come from? The first term serves to link x and p as canonical conjugates, and the second term is a restatement of the mass-shell constraint. But the last two terms don't seem to have any prior justification at all. Are they just thrown in there because they result in the Dirac equation? If so, the entire "derivation" is just a circular argument. If the last two terms are put in because of some more fundamental principle, what would that be?