Still Another Conservation Law — Question 1

Section 44-5 · Physics pages 7372–7373

Question 1 Associated production preserves strangeness in a strong collision For π−+ p →K0 + Λ, assign S=0 to the initial particles, S(K0) = +1 and S(Λ) = −1. Baryon numbers are 0 for mesons and 1 for baryons; both final particles are neutral. π−+ p K0 + Λ Schematic; labels, not drawing lengths, specify the data. (a) Check charge, baryon number and strangeness. (b) Explain why replacing the final state by π0 + Λ excludes a strong or electromagnetic reaction.
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Question 1 - Solution Associated production preserves strangeness in a strong collision π−+ p K0 + Λ (a) Method and calculation Q/e : −1 + 1 = 0 + 0, B : 0 + 1 = 0 + 1 . Si = 0, Sf = +1 −1 = 0 . (b) Interpretation and further calculation π0 + Λ : Sf = 0 −1 = −1 ⇒∆S = −1 . ∆S̸ = 0 ⇒not strong or electromagnetic . Physical check Strangeness is additive. Conservation permits the first channel but does not specify its cross section; weak interactions can change strangeness.

Question 1

Associated production preserves strangeness in a strong collision

For π−+p→K0+Λ\pi^-+p\to K^0+\Lambda, assign S=0 to the initial particles, S(K0)=+1S(K^0)=+1 and S(Λ)=−1S(\Lambda)=-1. Baryon numbers are 0 for mesons and 1 for baryons; both final particles are neutral.

Diagram shown in the original SVG worksheet.

  1. Check charge, baryon number and strangeness.

  2. Explain why replacing the final state by π0+Λ\pi^0+\Lambda excludes a strong or electromagnetic reaction.

Question 1 - Solution

Associated production preserves strangeness in a strong collision

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q/e:−1+1=0+0,B:0+1=0+1.\boxed{Q/e:\ -1+1=0+0,\quad B:\ 0+1=0+1}.Si=0,Sf=+1−1=0.\boxed{S_i=0,\quad S_f=+1-1=0}.

(b) Interpretation and further calculation

π0+Λ:Sf=0−1=−1⇒ΔS=−1.\pi^0+\Lambda:\quad S_f=0-1=-1\Rightarrow\boxed{\Delta S=-1}.ΔS≠0⇒not strong or electromagnetic.\boxed{\Delta S\ne0\Rightarrow\text{not strong or electromagnetic}}.

Physical check

Strangeness is additive. Conservation permits the first channel but does not specify its cross section; weak interactions can change strangeness.