Rules to compute Feynman Diagram with the Feynman rules

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SUMMARY

This discussion focuses on the computation of Feynman diagrams using Feynman rules, specifically addressing the importance of ordering factors due to non-commuting gamma matrices and spinors. Participants emphasize the necessity of labeling internal lines with momenta and following the particle flow direction. For electron-positron scattering (e+ e-), the order of computation does not matter, but it is crucial to ensure Lorentz invariance and to read diagrams from right to left, adhering to the direction of time.

PREREQUISITES
  • Understanding of Feynman diagrams and Feynman rules
  • Familiarity with gamma matrices and spinors
  • Knowledge of particle flow in quantum field theory
  • Basic principles of Lorentz invariance
NEXT STEPS
  • Study the process of labeling momenta in Feynman diagrams
  • Learn about the use of propagators in quantum field theory, specifically the fermionic propagator \(\frac{i (\not p + m)}{p^2-m^2}\)
  • Research the implications of Lorentz invariance in particle interactions
  • Explore the role of delta functions at vertices in Feynman diagrams
USEFUL FOR

Particle physicists, quantum field theorists, and students learning about Feynman diagrams and their computational techniques.

varphi42
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Hello,

I am trying to compute feynman diagrams with the feynman rules but I encounter some difficulties... Since the gamma matrices, spinnors, etc do not comute, the ordering of the different factor from feynman diagram has an importance. Is there some rules that say where to begin and in which order do we have to compute them?

I know for instance that we have to follow the particle flow but in the case of e+ e- scattering, do I begin with the e+ or the e-, etc ?

Thanks in advance
 
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Draw a diagram and read from right to left.time increases also in going from down to up.you should care to make amplitude lorentz invariant.it should be in order of increasing time.
I know for instance that we have to follow the particle flow but in the case of e+ e- scattering, do I begin with the e+ or the e-, etc ?
it does not matter.
 
My first step:
Label all internal lines with momenta.
Fermions : Label internal momenta in the DIRECTION OF THE ARROW, then use a regular
\frac{i (\not p + m)}{p^2-m^2}
propagator. Never think about internal fermions as antifermions/etc.
Bosons : I don't think it matters internally, so just choose whatever you want, I choose them so loops are directional. REALLY the delta functions at each vertex should take care of it.

Then I start at (for simple diagrams) the outgoing particles. (So start with things that are barred).

So for e+(p1) e-(p2) > gamma > e+(k1) e-(k2)


<br /> [\bar{u}_{k_2} (- i e Q_{\ell} \gamma_{\mu}) v_{k_1}] \times \left(-i \frac{g^{\mu \nu}}{q^2}\right) \times [\bar{v}_{p_1} (- i e Q_{\ell} \gamma_{\nu}) u_{p_2}]<br />
 
Draw a diagram and read from right to left
correction,it should read as we read from right to left,we just follow the arrows.
 

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