- #1
Rocky Raccoon
- 36
- 0
As is well known, a Dirac Lagrangian can be written in a symmetric form:
L = i/2 (\bar\psi \gamma \partial (\psi) - \partial (\bar\psi) \gamma \psi ) - m \bar\psi \psi
Let \psi and \psi^\dagger be independent fields. The corresponding canonical momenta are
p = i/2 \psi^\dagger;
p^\dagger = - i/2 \psi.
The anticommutation relations would be
{(\psi)_k, i/2 (\psi^dagger)_m}= i delta_km,
{(\psi^\dagger)_k, - i/2 (\psi)_m}= i delta_km,
which are in contradiction with one another. How can this happen?
L = i/2 (\bar\psi \gamma \partial (\psi) - \partial (\bar\psi) \gamma \psi ) - m \bar\psi \psi
Let \psi and \psi^\dagger be independent fields. The corresponding canonical momenta are
p = i/2 \psi^\dagger;
p^\dagger = - i/2 \psi.
The anticommutation relations would be
{(\psi)_k, i/2 (\psi^dagger)_m}= i delta_km,
{(\psi^\dagger)_k, - i/2 (\psi)_m}= i delta_km,
which are in contradiction with one another. How can this happen?