- #1
tommy01
- 40
- 0
Hi togehter.
I encountered the following problem:
The timeordering for fermionic fields (here Dirac field) is defined to be (Peskin; Maggiore, ...):
[tex]
T \Psi(x)\bar{\Psi}(y)= \Psi(x)\bar{\Psi}(y) \ldots x^0>y^0
[/tex]
[tex]
= -\bar{\Psi}(y)\Psi(x) \ldots y^0>x^0
[/tex]
where [tex]\Psi(x)[/tex] is a Dirac spinor and [tex]\bar{\Psi}(y) = \Psi(y)^\dagger \gamma^0[/tex] it's Dirac adjoint so that
[tex]
S(x-y) = \langle 0|T{ \Psi(x)\bar{\Psi}(y)}|0 \rangle
[/tex]
is the Feynman propagator which is a 4x4 matrix.
But there is my problem: while it is clear that [tex]\Psi(x)\bar{\Psi}(y)}[/tex] is a 4x4 matrix, [tex]\bar{\Psi}(y)\Psi(x)[/tex] is a scalar.
I would be glad for an explanation.
Thanks.
Tommy
I encountered the following problem:
The timeordering for fermionic fields (here Dirac field) is defined to be (Peskin; Maggiore, ...):
[tex]
T \Psi(x)\bar{\Psi}(y)= \Psi(x)\bar{\Psi}(y) \ldots x^0>y^0
[/tex]
[tex]
= -\bar{\Psi}(y)\Psi(x) \ldots y^0>x^0
[/tex]
where [tex]\Psi(x)[/tex] is a Dirac spinor and [tex]\bar{\Psi}(y) = \Psi(y)^\dagger \gamma^0[/tex] it's Dirac adjoint so that
[tex]
S(x-y) = \langle 0|T{ \Psi(x)\bar{\Psi}(y)}|0 \rangle
[/tex]
is the Feynman propagator which is a 4x4 matrix.
But there is my problem: while it is clear that [tex]\Psi(x)\bar{\Psi}(y)}[/tex] is a 4x4 matrix, [tex]\bar{\Psi}(y)\Psi(x)[/tex] is a scalar.
I would be glad for an explanation.
Thanks.
Tommy