The Basic Forces and Messenger Particles — Question 7

Section 44-8 · Physics pages 7444–7445

Question 7 A supplied running coupling decreases at shorter distances Use the one-loop-shaped model α(Q) = 1/[b ln(Q2/Λ2)], with b=.60 and Lambda=.20 GeV. Apply only for Q much larger than Lambda. Q α Schematic; labels, not drawing lengths, specify the data. (a) Calculate alpha at Q=2 and 20 GeV. (b) Find the coupling ratio and the ratio of rates proportional to alpha squared with other factors held fixed.
Show solutionHide solution
Question 7 - Solution A supplied running coupling decreases at shorter distances Q α (a) Method and calculation α(2) = 1/[.60 ln 100] = .361912 . α(20) = 1/[.60 ln 10000] = .180956 . (b) Interpretation and further calculation α(20)/α(2) = 1/2 . R20/R2 = (1/2)2 = 1/4 . Physical check This comparison isolates coupling dependence; actual cross sections also depend on energy, phase space and parton distributions. The model fails near its pole.

Question 7

A supplied running coupling decreases at shorter distances

Use the one-loop-shaped model α(Q)=1/[bln⁡(Q2/Λ2)]\alpha(Q)=1/[b\ln(Q^2/\Lambda^2)], with b=.60 and Lambda=.20 GeV. Apply only for Q much larger than Lambda.

Diagram shown in the original SVG worksheet.

  1. Calculate alpha at Q=2 and 20 GeV.

  2. Find the coupling ratio and the ratio of rates proportional to alpha squared with other factors held fixed.

Question 7 - Solution

A supplied running coupling decreases at shorter distances

Diagram shown in the original SVG worksheet.

(a) Method and calculation

α(2)=1/[.60ln⁡100]=.361912.\boxed{\alpha(2)=1/[.60\ln100]=.361912}.α(20)=1/[.60ln⁡10000]=.180956.\boxed{\alpha(20)=1/[.60\ln10000]=.180956}.

(b) Interpretation and further calculation

α(20)/α(2)=1/2.\boxed{\alpha(20)/\alpha(2)=1/2}.R20/R2=(1/2)2=1/4.\boxed{R_{20}/R_2=(1/2)^2=1/4}.

Physical check

This comparison isolates coupling dependence; actual cross sections also depend on energy, phase space and parton distributions. The model fails near its pole.