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The black vegetable
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- TL;DR Summary
- Using effective action to derive the one loop contribution of aa scalar field and fermion field
I am reading Peskin and Schroeder Section 11.4. They derive a formula for the effective action p.372 Equation 11.63 using a scalar field interaction,
They use this formula to determine the effective potential. If I want to do the same for a Lagrangian with with a scalar field and fermion field, can I use the same Formula reasoning and technique to get a formula for a scalar field and fermion field?
[tex]
\Gamma \left ( \phi _{cl} \right )=\int d^{4}L_{1}\left [ \phi _{cl} \right ]+\frac{i}{2}\log\text{Det}\left [ \frac{\partial ^{2}L_{1}}{\partial \phi \partial \phi } \right ] - i\: Connected\: Diagrams+\int d^{4}x\delta L\left [ \phi _{cl} \right ].\tag{11.63}
[/tex]
If so do you treat the Dirac Fermion [tex] \bar{\Psi } \Psi [/tex] as two different fields?
They use this formula to determine the effective potential. If I want to do the same for a Lagrangian with with a scalar field and fermion field, can I use the same Formula reasoning and technique to get a formula for a scalar field and fermion field?
[tex]
\Gamma \left ( \phi _{cl} \right )=\int d^{4}L_{1}\left [ \phi _{cl} \right ]+\frac{i}{2}\log\text{Det}\left [ \frac{\partial ^{2}L_{1}}{\partial \phi \partial \phi } \right ] - i\: Connected\: Diagrams+\int d^{4}x\delta L\left [ \phi _{cl} \right ].\tag{11.63}
[/tex]
If so do you treat the Dirac Fermion [tex] \bar{\Psi } \Psi [/tex] as two different fields?