Help W/ Calculating LSZ Formula for 2-2 Scattering Amplitude

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Discussion Overview

The discussion revolves around calculating a two to two scattering amplitude in the context of field theory, specifically using the LSZ formula and path integration techniques. Participants explore the contributions of various terms in the potential, particularly focusing on the polynomial form of the potential and its implications for the scattering amplitude.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant seeks assistance with calculating the scattering amplitude and notes that the answer should depend on the coefficients v2, v3, and v4 from the potential.
  • Another participant points out that while there is a four-point amplitude from the v4 term, contributions from v3 and v2 also arise from diagrams with internal lines connecting three-point vertices.
  • There is a discussion about the complexity of moving from the Lagrangian to the amplitude, with questions about whether the original poster is stuck on the LSZ part or the path integral evaluation.
  • A later reply indicates that the original poster realized their mistake was only considering first-order contributions, and acknowledges the need for second-order terms to include the v3 contribution.
  • Another participant notes the distinction between the orders of contributions from v4 and v3 in the coupling constant expansion.

Areas of Agreement / Disagreement

Participants generally agree on the need to consider multiple contributions to the scattering amplitude, particularly from different orders of the coupling constant. However, there is no explicit consensus on the specific steps or calculations involved in the process.

Contextual Notes

The discussion highlights the complexity of calculating scattering amplitudes and the importance of considering contributions from various terms in the potential, as well as the order of these contributions in the coupling constant expansion.

La Guinee
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I need some help getting started with calculating a two to two scattering amplitude (tree approximation) in the field theory with lagrangian:
g[tex]^{2}[/tex]L = ([tex]\partial[/tex][tex]\phi[/tex])[tex]^{2}[/tex] - V([tex]\phi[/tex])
where V is a polynomial in [tex]\phi[/tex]. That is,
V = [tex]\Sigma[/tex]v[tex]_{n}[/tex][tex]\phi^{n}[/tex]

I am trying to calculate this using techniques of path integration and the lsz formula. I know the answer depends only on v[tex]_{2}[/tex], v[tex]_{3}[/tex], and v[tex]_{4}[/tex] but I don't understand why. When I tried calculating the 4-point green's function I got it depending only on v[tex]_{4}[/tex] so I must be doing something wrong, but I don't know what.
 
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La Guinee said:
I need some help getting started with calculating a two to two scattering amplitude (tree approximation) in the field theory with lagrangian:
g[tex]^{2}[/tex]L = ([tex]\partial[/tex][tex]\phi[/tex])[tex]^{2}[/tex] - V([tex]\phi[/tex])
where V is a polynomial in [tex]\phi[/tex]. That is,
V = [tex]\Sigma[/tex]v[tex]_{n}[/tex][tex]\phi^{n}[/tex]

I am trying to calculate this using techniques of path integration and the lsz formula. I know the answer depends only on v[tex]_{2}[/tex], v[tex]_{3}[/tex], and v[tex]_{4}[/tex] but I don't understand why. When I tried calculating the 4-point green's function I got it depending only on v[tex]_{4}[/tex] so I must be doing something wrong, but I don't know what.

Can you post some of your steps?

Yes, there is a four point amplitude that comes from the V_4 term. But you should also get diagrams where there is an internal line connecting two three point vertex (like the tree level of the electron-positron scattering in QED). These will contain v_3 and v_2 (v_2 appearing in the propagator since it's essentially the mass of the scalr field, right?).

There are many many steps going from the lagrangian to an amplitude. Are you stuck with the LSZ part or in evaluating the amplitudes using path integrals? It's not clear where you are stuck, exactly.
 
kdv said:
Can you post some of your steps?

Yes, there is a four point amplitude that comes from the V_4 term. But you should also get diagrams where there is an internal line connecting two three point vertex (like the tree level of the electron-positron scattering in QED). These will contain v_3 and v_2 (v_2 appearing in the propagator since it's essentially the mass of the scalr field, right?).

There are many many steps going from the lagrangian to an amplitude. Are you stuck with the LSZ part or in evaluating the amplitudes using path integrals? It's not clear where you are stuck, exactly.

I actually figured it out. My mistake was that I was only going to first order. Like you said, you get a v_3 contribution from the second order term where you have an internal propagator. Thanks for the help.
 
La Guinee said:
I actually figured it out. My mistake was that I was only going to first order. Like you said, you get a v_3 contribution from the second order term where you have an internal propagator. Thanks for the help.

Good. I almost mentioned that in my post because the diagrams I described are clearly of order (v_3)^2 so they are of second order in the coupling constant but the diagrams are still tree level. So I almost mentioned the fact that the v_4 contribution and the v_3 contributions were of different order in the coupling constant expansion. But I decided to wait and hear back from you first.

Good for you.
 

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