Scattering Amplitudes BCFW relation (A question)

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SUMMARY

The discussion centers on the BCFW relation in the context of Yang-Mills (YM) theory, specifically addressing the sufficiency of 3-point amplitudes for determining n-point amplitudes at tree level. It is clarified that while 4-point amplitudes are essential for gauge invariance, the 3-point vertex can be used to construct n-point functions without tracking additional gauge degrees of freedom. The relationship between the coefficients of the 3-point and 4-point vertices is emphasized, highlighting their interconnectedness in YM theory.

PREREQUISITES
  • Understanding of Yang-Mills theory and its vertex functions
  • Familiarity with BCFW recursion relations
  • Knowledge of tree-level scattering amplitudes
  • Basic concepts of gauge invariance in quantum field theory
NEXT STEPS
  • Study the derivation of BCFW recursion relations in detail
  • Explore the role of gauge invariance in Yang-Mills Lagrangians
  • Investigate the implications of 4-point amplitudes in quantum field theories
  • Learn about the relationship between 3-point and 4-point vertex coefficients in various field theories
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The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, scattering amplitudes, and Yang-Mills theory, as well as graduate students seeking to deepen their understanding of these concepts.

AT80
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I have a very trivial question to ask and it would be great if someone could
help me in this.

The statement that '3-point amplitudes' and the location of poles are sufficient to
determine any n-point amplitude at tree level is confusing to me. Don't I also need to know
4-point amlitudes, for example in YM theory ? The reason I say this is
the 4-point vertex can not be broken down. That is the residues obtained upon putting
propagators onshell will also contain 4-point functions.

What am I missing ?

Thanks for your help in advance.
 
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In YM, the three point vertex coefficient and the four point coefficient are related to each other; one goes like g p_mu, and the other is g^2. The second is necessary to have a gauge-invariant Lagrangian. What's neat about YM is that given the three-point vertex at tree level, one can use it to build up the n-point function from BCFW, and you get the same answer as if you'd done Feynman rules, without having the miscellaneous gauge degrees of freedom to keep track of.

In a theory where the three- and four-point vertices were uncorrelated (scalar field theory with V = g phi^3 + lambda phi^4, for example), then you could BCFW up contributions to amplitudes that contained arbitrary powers of g, but no powers of lambda, using just the three-point function, but you wouldn't get the complete answer for the amplitudes. Hope this helps!
 
Thanks a lot Chrispb for a fast reply. It certainly helps.
 

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