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?
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?