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Lagrangian of $\phi^4$ theory

+ 1 like - 0 dislike
128 views

How do you derive the Lagrangian for a real scalar field ($\phi^4$ theory)?  I need to do so for spontaneous symmetry breaking. 

This question was asked by user34039 on Physics Stack Exchange but is now deleted there and has been restored from an archive.  

asked Mar 18, 2014 in Theoretical Physics by user34039 (5 points) [ revision history ]
edited Apr 30, 2014 by dimension10

What do you mean by derive? Do you mean to ask what it's physical interpretation is, and/or why someone would want to study it? - joshphysics  

No, I mean to derive it from first principles. - user34039

Which first principles? The way this business works is that either you (1) find a system and then determine if it can be well-described by a field theory you care about or (2) you say "let's consider this field theory" and then see if there is a system whose dynamics are governed by it, or perhaps a hybrid of the two. Which of these are you looking for in this context? FYI I'm not the downvoter. - joshphysics    

hybrid of the two - user34039

I suspect that what you mean is that you have a $Z_2$ symmetric theory $\mathcal{L} = -\frac12 (\partial\phi)^2+\frac12\mu^2\phi^2-\lambda\phi^4 $ and you would like to compute the Lagrangian appropriate for fluctuations about the phase where the $Z_2$ is spontaneously broken. You would want to write $\phi(x,t)=\bar\Phi + \varphi(x,t) $ where $\bar\Phi$ is the minimum of the potential $V\left(\phi\right) = - \frac12\mu^2\phi^2 +\lambda\phi^4  $. You can then plug this decomposition into $\mathcal L$, and keep all the terms that depend on $\varphi$. It's just algebra. - Andrew 

1 Answer

+ 2 like - 0 dislike

I suspect that what you mean is that you have a $Z_2$ symmetric theory $\mathcal{L} = -\frac12 (\partial\phi)^2+\frac12\mu^2\phi^2-\lambda\phi^4 $ and you would like to compute the Lagrangian appropriate for fluctuations about the phase where the $Z_2$ is spontaneously broken. You would want to write $\phi(x,t)=\bar\Phi + \varphi(x,t) $ where $\bar\Phi$ is the minimum of the potential $V\left(\phi\right) = - \frac12\mu^2\phi^2 +\lambda\phi^4  $. You can then plug this decomposition into $\mathcal L$, and keep all the terms that depend on $\varphi$. It's just algebra.  

answered Mar 18, 2014 by Andrew (135 points) [ revision history ]
edited Mar 23, 2014 by dimension10

This answer actually did not exist in the original PSE question, however, Andrew's comment was basically an answer, so I converted it. 

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