Beta Decay — Question 5

Section 42-5 · Physics pages 7080–7081

Question 5 Daughter recoil slightly lowers the beta endpoint For a beta-minus decay let Q=1.00 MeV and daughter rest energy Mc2 = 100000 MeV. At the electron endpoint the massless antineutrino energy tends to zero. Use p2 ec2 = Te(Te + 2mec2) and mec2 = .511 MeV. D e− endpoint: E¯ν →0 Schematic; labels, not drawing lengths, specify the data. (a) Derive the endpoint energy balance including nonrelativistic daughter recoil. (b) Evaluate the leading recoil correction by inserting Te ≃Q in the recoil term.
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Question 5 - Solution Daughter recoil slightly lowers the beta endpoint D e− endpoint: E¯ν →0 (a) Method and calculation pD = −pe ⇒TD = p2 e/(2M). Q = Te,max + Te,max(Te,max + 2mec2) 2Mc2 . (b) Interpretation and further calculation ∆T ≃Q(Q + 2mec2) 2Mc2 = 1.011 × 10−5 MeV = 10.11 eV . Te,max ≃.99998989 MeV . Physical check The endpoint is approached as neutrino energy vanishes. Recoil is small on a MeV scale but can matter in precision endpoint measurements.

Question 5

Daughter recoil slightly lowers the beta endpoint

For a beta-minus decay let Q=1.00 MeV and daughter rest energy Mc2=100000MeVMc^2=100000\,\mathrm{MeV}. At the electron endpoint the massless antineutrino energy tends to zero. Use pe2c2=Te(Te+2mec2)p_e^2c^2=T_e(T_e+2m_ec^2) and mec2=.511MeVm_ec^2=.511\,\mathrm{MeV}.

Diagram shown in the original SVG worksheet.

  1. Derive the endpoint energy balance including nonrelativistic daughter recoil.

  2. Evaluate the leading recoil correction by inserting Te≃QT_e\simeq Q in the recoil term.

Question 5 - Solution

Daughter recoil slightly lowers the beta endpoint

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝒑D=−𝒑e⇒TD=pe2/(2M).\mathbf p_D=-\mathbf p_e\Rightarrow T_D=p_e^2/(2M).Q=Te,max+Te,max(Te,max+2mec2)2Mc2.\boxed{Q=T_{e,\max}+\frac{T_{e,\max}(T_{e,\max}+2m_ec^2)}{2Mc^2}}.

(b) Interpretation and further calculation

ΔT≃Q(Q+2mec2)2Mc2=1.011×10−5MeV=10.11eV.\boxed{\Delta T\simeq\frac{Q(Q+2m_ec^2)}{2Mc^2}=1.011\times10^{-5}\,\mathrm{MeV}=10.11\,\mathrm{eV}}.Te,max≃.99998989MeV.\boxed{T_{e,\max}\simeq.99998989\,\mathrm{MeV}}.

Physical check

The endpoint is approached as neutrino energy vanishes. Recoil is small on a MeV scale but can matter in precision endpoint measurements.