The Photon, the Quantum of Light — Question 9

Section 38-1 · Physics pages 6268–6269

Question 9 A required detection probability determines the mean photon budget A weak pulse has Poisson-distributed incident photon number of mean µ. Each photon is detected independently with probability η = .200. The detected count is Poisson with mean ηµ. Require at least one detection with probability .950. Use hc = 1240 eV nm and 1 eV = 1.60 × 10−19 J. ηµ P(ND ≥1) Schematic; labels, not drawing lengths, specify the data. (a) Find the minimum incident mean photon number. (b) At wavelength 620 nm, find the required mean pulse energy and explain why a noninteger mean is admissible.
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Question 9 - Solution A required detection probability determines the mean photon budget ηµ P(ND ≥1) (a) Method and calculation P(ND ≥1) = 1 −P(ND = 0) = 1 −e−ηµ. 1 −e−.200µ ≥.950 ⇒ µ ≥5 ln 20 = 14.9787 . (b) Interpretation and further calculation U = µhc/λ = (5 ln 20)(3.20 × 10−19 J). Umin = 4.79317 × 10−18 J . Physical check Each individual count is an integer; the average over many pulses need not be.

Question 9

A required detection probability determines the mean photon budget

A weak pulse has Poisson-distributed incident photon number of mean μ\mu. Each photon is detected independently with probability η=.200\eta=.200. The detected count is Poisson with mean ημ\eta\mu. Require at least one detection with probability .950. Use hc=1240eVnmhc=1240\,\mathrm{eV\,nm} and 1eV=1.60×10−19J1\,\mathrm{eV}=1.60\times10^{-19}\,\mathrm J.

Diagram shown in the original SVG worksheet.

  1. Find the minimum incident mean photon number.

  2. At wavelength 620 nm, find the required mean pulse energy and explain why a noninteger mean is admissible.

Question 9 - Solution

A required detection probability determines the mean photon budget

Diagram shown in the original SVG worksheet.

(a) Method and calculation

P(ND≥1)=1−P(ND=0)=1−e−ημ.P(N_D\ge1)=1-P(N_D=0)=1-e^{-\eta\mu}.1−e−.200μ≥.950⇒μ≥5ln⁡20=14.9787.1-e^{-.200\mu}\ge.950\quad\Rightarrow\quad\boxed{\mu\ge5\ln20=14.9787}.

(b) Interpretation and further calculation

U¯=μhc/λ=(5ln⁡20)(3.20×10−19J).\overline U=\mu hc/\lambda=(5\ln20)(3.20\times10^{-19}\,\mathrm J).U¯min=4.79317×10−18J.\boxed{\overline U_{\min}=4.79317\times10^{-18}\,\mathrm J}.

Physical check

Each individual count is an integer; the average over many pulses need not be.