Still Another Conservation Law — Question 2

Section 44-5 · Physics pages 7374–7375

Question 2 A strange baryon can decay weakly even when strong decay is excluded For Λ →p + π−take rest energies 1116, 938 and 140 MeV. The Lambda has S=-1 and both daughters have S=0. Baryon number and charge are conserved. Λ p + π− Schematic; labels, not drawing lengths, specify the data. (a) Find Q and strangeness change, and identify the required interaction class. (b) Estimate daughter momentum using the nonrelativistic relative-energy relation Q = p2/(2µ), with reduced mass µ = mpmπ/(mp + mπ). Check the approximation.
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Question 2 - Solution A strange baryon can decay weakly even when strong decay is excluded Λ p + π− (a) Method and calculation Q = 1116 −938 −140 = 38 MeV, ∆S = +1 . weak decay required despite positive Q. (b) Interpretation and further calculation µc2 = 938(140) 1078 = 121.818 MeV, pc ≃ √ 2µc2Q = 96.219 MeV . pc/(mπc2) ≃.687 so the pion is not deeply nonrelativistic. Physical check The momentum is explicitly a rough estimate, not an accurate decay prediction. Positive energy release alone does not determine the decay mechanism.

Question 2

A strange baryon can decay weakly even when strong decay is excluded

For Λ→p+π−\Lambda\to p+\pi^- take rest energies 1116, 938 and 140 MeV. The Lambda has S=-1 and both daughters have S=0. Baryon number and charge are conserved.

Diagram shown in the original SVG worksheet.

  1. Find Q and strangeness change, and identify the required interaction class.

  2. Estimate daughter momentum using the nonrelativistic relative-energy relation Q=p2/(2μ)Q=p^2/(2\mu), with reduced mass μ=mpmπ/(mp+mπ)\mu=m_pm_\pi/(m_p+m_\pi). Check the approximation.

Question 2 - Solution

A strange baryon can decay weakly even when strong decay is excluded

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q=1116−938−140=38MeV,ΔS=+1.\boxed{Q=1116-938-140=38\,\mathrm{MeV},\quad\Delta S=+1}.weak decay requireddespite positive Q.\boxed{\text{weak decay required}}\quad\text{despite positive }Q.

(b) Interpretation and further calculation

μc2=938(140)1078=121.818MeV,pc≃2μc2Q=96.219MeV.\mu c^2=\frac{938(140)}{1078}=121.818\,\mathrm{MeV},\quad\boxed{pc\simeq\sqrt{2\mu c^2Q}=96.219\,\mathrm{MeV}}.pc/(mπc2)≃.687so the pion is not deeply nonrelativistic.\boxed{pc/(m_\pi c^2)\simeq.687}\quad\text{so the pion is not deeply nonrelativistic}.

Physical check

The momentum is explicitly a rough estimate, not an accurate decay prediction. Positive energy release alone does not determine the decay mechanism.