The Leptons — Question 6

Section 44-3 · Physics pages 7342–7343

Question 6 A neutrino oscillation minimum measures mass-squared splitting Use a two-flavor survival model Pµµ = 1 −sin2(2θ) sin2(1.27∆m2L/E), with ∆m2 in eV squared, L in km and E in GeV. Set sin2(2θ) = 1, ∆m2 = 2.50 × 10−3 eV2 and E=1.00 GeV. L Pµµ Schematic; labels, not drawing lengths, specify the data. (a) Find the first positive baseline giving minimum survival. (b) Find survival at half that baseline and explain why the experiment measures a mass-squared difference rather than an absolute mass.
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Question 6 - Solution A neutrino oscillation minimum measures mass-squared splitting L Pµµ (a) Method and calculation 1.27∆m2Lmin/E = π/2. Lmin = π(1.00) 2(1.27)(.00250) = 494.739 km . (b) Interpretation and further calculation Pµµ(Lmin/2) = 1 −sin2(π/4) = .500 . m2 1 →m2 1 + C, m2 2 →m2 2 + C leaves ∆m2 unchanged. Physical check This vacuum two-flavor approximation omits matter effects and the third flavor. Oscillations require distinct propagation phases.

Question 6

A neutrino oscillation minimum measures mass-squared splitting

Use a two-flavor survival model Pμμ=1−sin⁡2(2θ)sin⁡2(1.27Δm2L/E)P_{\mu\mu}=1-\sin^2(2\theta)\sin^2(1.27\Delta m^2L/E), with Δm2\Delta m^2 in eV squared, L in km and E in GeV. Set sin⁡2(2θ)=1\sin^2(2\theta)=1, Δm2=2.50×10−3eV2\Delta m^2=2.50\times10^{-3}\,\mathrm{eV^2} and E=1.00 GeV.

Diagram shown in the original SVG worksheet.

  1. Find the first positive baseline giving minimum survival.

  2. Find survival at half that baseline and explain why the experiment measures a mass-squared difference rather than an absolute mass.

Question 6 - Solution

A neutrino oscillation minimum measures mass-squared splitting

Diagram shown in the original SVG worksheet.

(a) Method and calculation

1.27Δm2Lmin/E=π/2.1.27\Delta m^2L_{\min}/E=\pi/2.Lmin=π(1.00)2(1.27)(.00250)=494.739km.\boxed{L_{\min}=\frac{\pi(1.00)}{2(1.27)(.00250)}=494.739\,\mathrm{km}}.

(b) Interpretation and further calculation

Pμμ(Lmin/2)=1−sin⁡2(π/4)=.500.\boxed{P_{\mu\mu}(L_{\min}/2)=1-\sin^2(\pi/4)=.500}.m12→m12+C,m22→m22+Cleaves Δm2 unchanged.\boxed{m_1^2\to m_1^2+C,\ m_2^2\to m_2^2+C}\quad\text{leaves }\Delta m^2\text{ unchanged}.

Physical check

This vacuum two-flavor approximation omits matter effects and the third flavor. Oscillations require distinct propagation phases.