Calc Feynman Amp Q: Chi+ Chi- -> Chi+ Chi-

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SUMMARY

The Feynman amplitude for the scalar scattering process \(\chi^+ \chi^- \to \chi^+ \chi^-\) is calculated using the interaction Lagrangian \(\mathcal{L} = - g \chi^\dagger \chi \Phi - \frac{\lambda}{4} (\chi^\dagger \chi)^2\). The total amplitude is expressed as \((-ig)^2 \left(\frac{i}{(p_1 + p_2)^2 - M^2} + \frac{i}{(p_1 - k_1)^2 - M^2} \right) - \frac{i\lambda}{4}\), where \(M\) is the mass of the \(\Phi\) boson, and \(p_1, p_2, k_1, k_2\) represent the energy-momenta of the particles. There are two Feynman diagrams for the interaction term \(g \chi^\dagger \chi \Phi\) and one for the quartic term \(\lambda (\chi^\dagger \chi)^2\).

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  • Understanding of Feynman diagrams and their construction
  • Knowledge of scalar field theory and interaction Lagrangians
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Particle physicists, quantum field theorists, and students studying scattering processes in high-energy physics will benefit from this discussion.

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I'm having a problem calculating the Feynman amplitude for the scalar scattering process [tex]\chi^+ \chi^- \to \chi^+ \chi^-[/tex] for an interaction Lagrangian which is:

[tex]\mathcal{L} = - g \chi^\dagger \chi \Phi - \frac{\lambda}{4} (\chi^\dagger \chi)^2[/tex]

So far I have the 2 Feynman Diagrams for [tex]\chi^+ \chi^- \to \Phi \to \chi^+ \chi^-[/tex] but I can't think/remember how many there should be for the quartic term. I'm thinking there should only be one diagram and hence only one contribution to the Feynman amplitude (which should be -i lambda/4), so the total amplitude becomes:

[tex](-ig)^2 \left(\frac{i}{(p_1 + p_2)^2 - M^2} + \frac{i}{(p_1 - k_1)^2 - M^2} \right) - \frac{i\lambda}{4}[/tex]

where M is the mass of Phi boson, p_1 and p_2 are the incoming energy-momenta and k_1 and k_2 are the outgoing energy-momenta.

Am I along the right lines?

Thanks
 
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in advance!Yes, you are on the right track. The Feynman amplitude for the scalar scattering process $\chi^+ \chi^- \to \chi^+ \chi^-$ is given by: \begin{align}i\mathcal{M} = (-ig)^2 \left(\frac{i}{(p_1 + p_2)^2 - M^2} + \frac{i}{(p_1 - k_1)^2 - M^2} \right) - \frac{i\lambda}{4}.\end{align}This is due to the fact that there will be two diagrams for the interaction term $g \chi^\dagger \chi \Phi$ and only one diagram for the quartic term $\lambda (\chi^\dagger \chi)^2$.
 

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