A Pause for Reflection — Question 7

Section 44-9 · Physics pages 7464–7465

Question 7 A tiny reconstructed mass is sensitive to the opening-angle calibration Two photons of equal energy E=10 GeV have small opening angle theta=.020 rad, with uncertainty .002 rad. Energy uncertainties are negligible. γ1 γ2 small θ Schematic; labels, not drawing lengths, specify the data. (a) Use the exact invariant relation to derive the small-angle mass formula and estimate M. (b) Propagate the angle uncertainty and compare its fractional size with a 1 percent common energy-scale error.
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Question 7 - Solution A tiny reconstructed mass is sensitive to the opening-angle calibration γ1 γ2 small θ (a) Method and calculation M2 = 2E2(1 −cos θ) ≃E2θ2. M ≃Eθ = .200 GeV/c2 (c = 1 in the derivation). (b) Interpretation and further calculation σM ≃Eσθ = .020 GeV/c2, σM/M = .10 . δM/M = δE/E = .01 for a common energy-scale shift. Physical check The angle uncertainty dominates this example. Nearly collinear photons make a small invariant mass despite a large total laboratory energy.

Question 7

A tiny reconstructed mass is sensitive to the opening-angle calibration

Two photons of equal energy E=10 GeV have small opening angle theta=.020 rad, with uncertainty .002 rad. Energy uncertainties are negligible.

Diagram shown in the original SVG worksheet.

  1. Use the exact invariant relation to derive the small-angle mass formula and estimate M.

  2. Propagate the angle uncertainty and compare its fractional size with a 1 percent common energy-scale error.

Question 7 - Solution

A tiny reconstructed mass is sensitive to the opening-angle calibration

Diagram shown in the original SVG worksheet.

(a) Method and calculation

M2=2E2(1−cos⁡θ)≃E2θ2.M^2=2E^2(1-\cos\theta)\simeq E^2\theta^2.M≃Eθ=.200GeV/c2(c=1 in the derivation).\boxed{M\simeq E\theta=.200\ {\mathrm{GeV}}/c^2}\quad(c=1\text{ in the derivation}).

(b) Interpretation and further calculation

σM≃Eσθ=.020GeV/c2,σM/M=.10.\boxed{\sigma_M\simeq E\sigma_\theta=.020\ {\mathrm{GeV}}/c^2,\quad\sigma_M/M=.10}.δM/M=δE/E=.01for a common energy-scale shift.\boxed{\delta M/M=\delta E/E=.01}\quad\text{for a common energy-scale shift}.

Physical check

The angle uncertainty dominates this example. Nearly collinear photons make a small invariant mass despite a large total laboratory energy.