How Does the Mass of the Bottom Quark Affect Z Boson Decay Calculations?

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Discussion Overview

The discussion revolves around the impact of the bottom quark mass on the calculations of the Z boson decay partial width. Participants explore theoretical and experimental aspects of this topic, including the implications of not neglecting the bottom quark mass in decay calculations.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions the effects of including the bottom quark mass in Z boson decay calculations, noting that theoretical calculations typically assume negligible masses for decay products.
  • Another participant asserts that neglecting the mass would lead to identical predictions for all quarks, which contradicts experimental results that show differences.
  • A subsequent post inquires about the nature of corrections that would arise from considering the bottom quark mass, specifically whether these corrections would increase or decrease the partial width.
  • Reference to a source indicates that the mass of the bottom quark appears to increase the partial decay width, although the complexities of hadronization are acknowledged.
  • One participant estimates that the theoretical effect of the bottom quark mass on the decay width is around 1%, aligning with observed differences and uncertainties.
  • A challenge is raised regarding the source of the 1% figure, with a specific branching fraction provided that highlights a small uncertainty compared to a proposed value.
  • Discussion includes a mention of phase space factors and loop effects that contribute to the decay calculations, suggesting a need for careful comparison of branching fractions among different quark pairs.

Areas of Agreement / Disagreement

Participants express differing views on the implications of including the bottom quark mass in decay calculations, with no consensus reached on the exact effects or the validity of specific numerical estimates.

Contextual Notes

Limitations include potential dependencies on the definitions of decay widths and branching fractions, as well as unresolved mathematical steps in the calculations discussed.

Catria
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Hello everyone,

I have read about the theoretical values of the Z boson decay partial width and how well they agreed with experiment. However there is something I do not quite understand: since these theoretical calculations were performed with the hypothesis that the masses of the decay products were negligible with respect to the mass of the Z boson, what changes would have to be effected if one did not neglect the mass of the bottom quark (~4-5 GeV) when computing the partial width of the Z boson into a bottom and anti-bottom quark pair?
 
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If the theoretical calculations would not take the mass into account, they would predict the same values for all quarks. They do not, and the predicted difference has been confirmed by experiment.
 
Then, what... form would these corrections take? Would those corrections for the bottom quark have the effect of increasing or decreasing the partial width?
 
Based on the http://pdg8.lbl.gov/rpp2013v2/pdgLive/Particle.action?node=S044 , it looks like mass is increasing the partial decay width. Hadronization makes it tricky to disentangle the light quarks, but bb gets more than 1/5 of the hadronic decay width.
 
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The theoretical effect will be something around 1%. The observational difference is about 1% with an uncertainty of about half a percent.
 
How did you get those numbers? Γ(Z → bb¯ )/Γ(Z → hadrons ) is given as 0.21629 ± 0.00066 where bold highlights matching digits. The uncertainty is tiny compared to the difference to 0.2.
 
The phase space factor is about a percent. This can be accurately calculated, since its a ratio.

The absolute branching fraction to hadrons has loop effects (color connection) of the order alpha_s/16 pi, or again a good fraction of a percent. So one would need to compare Γ(Z → bb)/[Γ(Z → bb) + Γ(Z → dd) + Γ(Z → ss)] which what I did and is good to half a percent. Your suggestion to lump all the hadrons together is interesting, but it would require taking the weak mixing angle measurement from some other experiment, so one could constrain Γ(Z → uu)/[Γ(Z → dd). I'd have to look more closely to see if you win or not with this.
 

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