What's the classical picture of phi^4 scalar field theory?

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SUMMARY

The classical picture of phi^4 scalar field theory indicates that particles repel each other due to the potential energy associated with the phi^4 term, which grows faster than phi^2. This repulsion arises from the energetic unlikelihood of particles clumping together, as larger amplitudes are energetically unfavorable. The interaction's nature—whether attractive or repulsive—depends on the sign of the delta potential, which is influenced by the coefficient of the phi^4 term in the Lagrangian. This understanding is not commonly addressed in introductory field theory texts, such as Peskin & Schroder.

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  • Understanding of scalar field theory concepts
  • Familiarity with Lagrangian mechanics
  • Knowledge of potential energy in quantum field theory
  • Basic grasp of scattering amplitudes and delta potentials
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  • Study the implications of the phi^4 potential in quantum field theory
  • Explore the derivation of scattering amplitudes in scalar field theories
  • Investigate the role of the Lagrangian in determining particle interactions
  • Review classical field theory texts for insights on phi^4 interactions
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Physicists, particularly those specializing in quantum field theory, students of theoretical physics, and anyone interested in the dynamics of scalar fields and particle interactions.

petergreat
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I know that the classical picture of QED is Coulomb interaction, magnetic interaction etc. But what does the classical phi^4 theory look like? In particular, do particles attract or repel each other in this theory?

P.S. I'm surprised that my field theory books never discuss this. (At least in Peskin & Schroder's introductory chapter on scalar field theory.)
 
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have you tried work it out for yourself?
 
My intuition is that particles will repel each other to separate apart, because clumping together and forming large amplitudes is energetically unfavorable due to the phi^4 potential which grows faster than phi^2. Is this correct? I'll try to do some math when I have time.
 
For \phi\phi \rightarrow \phi\phi scattering, I think the scattering amplitude translates into a delta potential between the two mesons.

Whether the interaction is attractive or repulsive will depend on the sign of the delta potential which then depends on the coefficient of \phi^4 in the Lagrangian.



I'm pretty sure that I saw this somewhere in a (non-advanced) field theory text. But correct me if what I said was wrong.
 

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