X Rays and the Ordering of the Elements — Question 8

Section 40-9 · Physics pages 6746–6747

Question 8 A fluorescence yield converts a vacancy rate into a photon count K vacancies are created at rate RK = 2.00 × 108 s−1. The radiative yield is ωK = .40, and .80 of radiative decays produce Kα. A detector subtends .010 of the full solid angle and has quantum efficiency .60. Assume isotropic emission and no absorption. photons detector RKωKbα Schematic; labels, not drawing lengths, specify the data. (a) Find the emitted Kα rate and detected count rate. (b) Find the expected counts in .250 s and the Poisson relative standard deviation.
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Question 8 - Solution A fluorescence yield converts a vacancy rate into a photon count photons detector RKωKbα (a) Method and calculation Rα = RKωKbα = (2.00 × 108)(.40)(.80) = 6.40 × 107 s−1 . Rd = Rα(.010)(.60) = 3.84 × 105 s−1 . (b) Interpretation and further calculation ¯N = Rdt = 9.60 × 104 . σN = √¯N ⇒σN/ ¯N = 1/ √ 96000 = .003227 . Physical check The nonradiative fraction and other radiative branches are removed before applying detector acceptance and efficiency. Poisson statistics assume independent events and negligible dead time.

Question 8

A fluorescence yield converts a vacancy rate into a photon count

K vacancies are created at rate RK=2.00×108s−1R_K=2.00\times10^8\,\mathrm{s^{-1}}. The radiative yield is ωK=.40\omega_K=.40, and .80 of radiative decays produce KαK_\alpha. A detector subtends .010 of the full solid angle and has quantum efficiency .60. Assume isotropic emission and no absorption.

Diagram shown in the original SVG worksheet.

  1. Find the emitted KαK_\alpha rate and detected count rate.

  2. Find the expected counts in .250 s and the Poisson relative standard deviation.

Question 8 - Solution

A fluorescence yield converts a vacancy rate into a photon count

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Rα=RKωKbα=(2.00×108)(.40)(.80)=6.40×107s−1.R_\alpha=R_K\omega_Kb_\alpha=(2.00\times10^8)(.40)(.80)=\boxed{6.40\times10^7\,\mathrm{s^{-1}}}.Rd=Rα(.010)(.60)=3.84×105s−1.\boxed{R_d=R_\alpha(.010)(.60)=3.84\times10^5\,\mathrm{s^{-1}}}.

(b) Interpretation and further calculation

N‾=Rdt=9.60×104.\boxed{\bar N=R_dt=9.60\times10^4}.σN=N‾⇒σN/N‾=1/96000=.003227.\sigma_N=\sqrt{\bar N}\Rightarrow\boxed{\sigma_N/\bar N=1/\sqrt{96000}=.003227}.

Physical check

The nonradiative fraction and other radiative branches are removed before applying detector acceptance and efficiency. Poisson statistics assume independent events and negligible dead time.