Quantum Field Theory: Stationary Point of the Effective Action

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latentcorpse
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We have the effective action which obeys [itex]\frac{\delta \Gamma[\varphi]}{\delta \varphi(x)}=J(x)[/itex] where and we are told the stationary point, [itex]\varphi_0[/itex], of this action, [itex]\frac{\delta \Gamma[\varphi_0]}{\delta \varphi(x)}=0[/itex], corresponds to the vacuum expectation value.
(This is out of my notes - there is a discussion around p380 of Peskin & Schroeder on this although it goes a bit more in depth than my notes...)

Anyway, on the next page, he just says that we can write

[itex]\Gamma[\varphi]=i \displaystyle\sum_{n=0}^\infty \frac{1}{n!} \int d^dx_1 \dots \int d^dx_n \varphi(x_1) \dots \varphi(x_n) \Gamma_n (x_1, \dots , x_n)[/itex]

Can anybody explain to me where this formula has come from? And what is [itex]\Gamma_n[/itex]? He hasn't defined that either.

Thanks.
 
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Up to the factor of [tex]i[/tex] this is just a power-series expansion for a functional. [tex]\Gamma_n[/tex] can be expressed in terms of functional derivatives of [tex]\Gamma[/tex] evaluated at [tex]\phi = 0[/tex] as written.
 
fzero said:
Up to the factor of [tex]i[/tex] this is just a power-series expansion for a functional. [tex]\Gamma_n[/tex] can be expressed in terms of functional derivatives of [tex]\Gamma[/tex] evaluated at [tex]\phi = 0[/tex] as written.

Ok. So I found that [itex]\Gamma_n = - i \frac{\delta^n \Gamma [ \varphi ] }{ \delta \varphi(x_1) \dots \delta \varphi(x_n)}|_{\varphi=0}[/itex]

But shouldn't this be evaluated at [itex]\varhpi = \varphi_0[/itex] i.e. the minimum of the effective potential?
 
latentcorpse said:
Ok. So I found that [itex]\Gamma_n = - i \frac{\delta^n \Gamma [ \varphi ] }{ \delta \varphi(x_1) \dots \delta \varphi(x_n)}|_{\varphi=0}[/itex]

But shouldn't this be evaluated at [itex]\varhpi = \varphi_0[/itex] i.e. the minimum of the effective potential?

The whole expansion should be made around [tex]\varphi=\varphi_0[/tex]. Your reference is either being sloppy or you've left out information.