Still Another Conservation Law — Question 5

Section 44-5 · Physics pages 7380–7381

Question 5 A cascade removes strangeness in separate weak steps Consider Ξ−→Λ + π−followed by Λ →p + π−. Assign S=-2,-1,0 to Xi, Lambda and proton, and S=0 to pions. Proper waiting times in the two rest frames are independent exponential variables with means 1.60 and 2.60 units of 10−10 s. Ξ− Λ + π−→p + 2π− Schematic; labels, not drawing lengths, specify the data. (a) Write the net final state and the strangeness change in each step. (b) For the sum of the two proper waiting-time variables, find mean and standard deviation. Explain why it is not automatically a laboratory transit time.
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Question 5 - Solution A cascade removes strangeness in separate weak steps Ξ− Λ + π−→p + 2π− (a) Method and calculation Ξ−→p + 2π−, ∆S1 = +1, ∆S2 = +1 . Q/e : −1 = 1 −2, B : 1 = 1, ∆Snet = +2 . (b) Interpretation and further calculation ⟨T1 + T2⟩= (1.60 + 2.60)10−10 = 4.20 × 10−10 s . σT1+T2 = √ 1.602 + 2.602 10−10 = 3.05287 × 10−10 s . Physical check The two proper times refer to different moving particles. Laboratory durations require their separate Lorentz factors.

Question 5

A cascade removes strangeness in separate weak steps

Consider Ξ−→Λ+π−\Xi^-\to\Lambda+\pi^- followed by Λ→p+π−\Lambda\to p+\pi^-. Assign S=-2,-1,0 to Xi, Lambda and proton, and S=0 to pions. Proper waiting times in the two rest frames are independent exponential variables with means 1.60 and 2.60 units of 10−1010^{-10} s.

Diagram shown in the original SVG worksheet.

  1. Write the net final state and the strangeness change in each step.

  2. For the sum of the two proper waiting-time variables, find mean and standard deviation. Explain why it is not automatically a laboratory transit time.

Question 5 - Solution

A cascade removes strangeness in separate weak steps

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ξ−→p+2π−,ΔS1=+1,ΔS2=+1.\boxed{\Xi^-\to p+2\pi^-,\quad\Delta S_1=+1,\quad\Delta S_2=+1}.Q/e:−1=1−2,B:1=1,ΔSnet=+2.Q/e:\ -1=1-2,\quad B:\ 1=1,\quad\boxed{\Delta S_{\mathrm{net}}=+2}.

(b) Interpretation and further calculation

⟨T1+T2⟩=(1.60+2.60)10−10=4.20×10−10s.\boxed{\langle T_1+T_2\rangle=(1.60+2.60)10^{-10}=4.20\times10^{-10}\,\mathrm s}.σT1+T2=1.602+2.60210−10=3.05287×10−10s.\boxed{\sigma_{T_1+T_2}=\sqrt{1.60^2+2.60^2}\,10^{-10}=3.05287\times10^{-10}\,\mathrm s}.

Physical check

The two proper times refer to different moving particles. Laboratory durations require their separate Lorentz factors.