Supression factor for triangle diagrams

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SUMMARY

The discussion focuses on the suppression factors associated with triangle diagrams in particle physics, specifically comparing the processes H→γγ and H→b b̅. The participant analyzes the contributions of different vertices, noting that H→γγ involves two WWγ vertices and a W propagator, while H→b b̅ has two Wbb vertices and a fermion propagator. The conclusion drawn is that H→γγ is expected to be more suppressed than H→b b̅, but the participant realizes that the absence of a Wbb vertex and the presence of CKM suppression factors complicate this analysis. Ultimately, the participant acknowledges that the top quark's propagator introduces a larger suppression than that of the bottom quark.

PREREQUISITES
  • Understanding of triangle diagrams in particle physics
  • Familiarity with the Higgs boson decay processes
  • Knowledge of CKM (Cabibbo-Kobayashi-Maskawa) matrix and its implications
  • Basic concepts of particle propagators and their suppression effects
NEXT STEPS
  • Research the role of CKM matrix elements in particle decay processes
  • Study the implications of different propagators in quantum field theory
  • Examine the cutting rules in Feynman diagrams for particle interactions
  • Explore the differences in suppression factors between various Higgs decay channels
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Particle physicists, graduate students in theoretical physics, and researchers analyzing Higgs boson decay mechanisms will benefit from this discussion.

frizzie
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I'm pretty shaky with my understanding of much beyond simple tree-level calculations. When people talk about triangle diagrams, they sometimes say one will get a 'supression factor' of xxx. For example, in the consider the triangle diagram for H\rightarrow\gamma\gamma with Ws running around the loop (attached). I want to know, without doing the full calculation, whether that would be more or less suppressed than second-order H\rightarrow b \bar{b} (the same triangle diagram, except with bottom quark external legs instead of photons and a quark where the vertical W is.)

My thought was that you can use the cutting rules, so the relevant difference between the two is that H\rightarrow\gamma\gamma has two WW\gamma vertices and a W propagator, and H\rightarrow b \bar{b} has two Wbb vertices and a fermion propagator. But plugging everything in, I get that H\rightarrow\gamma\gamma should be more suppressed than second-order H\rightarrow b \bar{b}, which isn't correct. Does my approach make any sense?
 

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Hmm, well there is no such vertex as Wbb. W's change up type quarks to down types and vice versa, so the quark in the loop must be some up type quark. So you have a CKM suppression factor in each of those vertices also. Although it will probably just be a top quark in the loop and I think the CKM factor V_tb is practically 1 so this is not too much of a bother. I suppose also that the top propagator is a bigger suppression than the bottom one so there is that too.
 

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