Still Another Conservation Law — Question 6

Section 44-5 · Physics pages 7382–7383

Question 6 Associated strangeness production has a center-of-mass mass threshold For π−+ p →K0 + Λ on a stationary proton, use rest energies mπ = .140, mp = .940, mK = .500 and mΛ = 1.120 GeV, with c=1. The channel conserves Q, B and S. π−+ p K0 + Λ Schematic; labels, not drawing lengths, specify the data. (a) Calculate the threshold total energy of the incident pion. (b) Find its threshold kinetic energy and compare with the rest-energy increase of the reaction.
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Question 6 - Solution Associated strangeness production has a center-of-mass mass threshold π−+ p K0 + Λ (a) Method and calculation W 2 = m2 π + m2 p + 2mpEπ, Wth = mK + mΛ = 1.620 GeV. Eπ,th = 1.6202 −.1402 −.9402 2(.940) = .915532 GeV . (b) Interpretation and further calculation Kπ,th = .775532 GeV . ∆Erest = 1.620 −(.140 + .940) = .540 GeV < Kπ,th . Physical check Passing strangeness conservation does not remove the kinematic threshold. The difference is associated with motion of the final center of mass.

Question 6

Associated strangeness production has a center-of-mass mass threshold

For π−+p→K0+Λ\pi^-+p\to K^0+\Lambda on a stationary proton, use rest energies mπ=.140m_\pi=.140, mp=.940m_p=.940, mK=.500m_K=.500 and mΛ=1.120m_\Lambda=1.120 GeV, with c=1. The channel conserves Q, B and S.

Diagram shown in the original SVG worksheet.

  1. Calculate the threshold total energy of the incident pion.

  2. Find its threshold kinetic energy and compare with the rest-energy increase of the reaction.

Question 6 - Solution

Associated strangeness production has a center-of-mass mass threshold

Diagram shown in the original SVG worksheet.

(a) Method and calculation

W2=mπ2+mp2+2mpEπ,Wth=mK+mΛ=1.620GeV.W^2=m_\pi^2+m_p^2+2m_pE_\pi,\quad W_{\mathrm{th}}=m_K+m_\Lambda=1.620\,\mathrm{GeV}.Eπ,th=1.6202−.1402−.94022(.940)=.915532GeV.\boxed{E_{\pi,\mathrm{th}}=\frac{1.620^2-.140^2-.940^2}{2(.940)}=.915532\,\mathrm{GeV}}.

(b) Interpretation and further calculation

Kπ,th=.775532GeV.\boxed{K_{\pi,\mathrm{th}}=.775532\,\mathrm{GeV}}.ΔErest=1.620−(.140+.940)=.540GeV<Kπ,th.\boxed{\Delta E_{\mathrm{rest}}=1.620-(.140+.940)=.540\,\mathrm{GeV}<K_{\pi,\mathrm{th}}}.

Physical check

Passing strangeness conservation does not remove the kinematic threshold. The difference is associated with motion of the final center of mass.