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Student Friendly Introduction to QFT
· Problem 22
Spinors: Spin ½ Fields
Physics — QFT · euler-lagrange-dirac-lagrangian
Problem
Prove to yourself that for
n
=
1
n = 1
n
=
1
in the Euler-Lagrange equation applied to the Dirac Lagrangian density
L
0
1
/
2
=
ψ
ˉ
(
i
γ
α
∂
α
−
m
)
ψ
\mathcal{L}_0^{1/2} = \bar{\psi}(i\gamma^\alpha \partial_\alpha - m)\psi
L
0
1/2
=
ψ
ˉ
(
i
γ
α
∂
α
−
m
)
ψ
, we get the Dirac equation, and for
n
=
2
n = 2
n
=
2
, we get the adjoint Dirac equation.
Related theory
Lagrangian Mechanics Simple Pendulum Via Euler Lagrange
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