The Photon, the Quantum of Light — Question 6

Section 38-1 · Physics pages 6262–6263

Question 6 Frequency doubling conserves energy rather than photon number A lossless idealized frequency doubler converts pairs of input photons at frequency f into single photons at 2f. For a real device, a fraction η = .800 of incident optical power emerges in the doubled-frequency beam; the rest remains at f. f 2f f Schematic; labels, not drawing lengths, specify the data. (a) Find doubled-frequency and residual photon rates in terms of input rate ˙N. (b) Find the total output photon rate and verify energy conservation.
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Question 6 - Solution Frequency doubling conserves energy rather than photon number f 2f f (a) Method and calculation 2hf ˙N2f = ηhf ˙N ⇒ ˙N2f = .400 ˙N . hf ˙Nf = (1 −η)hf ˙N ⇒ ˙Nf = .200 ˙N . (b) Interpretation and further calculation ˙Nout = .600 ˙N . Pout = hf(.200 ˙N) + 2hf(.400 ˙N) = hf ˙N = Pin . Physical check Photon number need not be conserved in a nonlinear optical conversion, while the stated energy accounting must hold.

Question 6

Frequency doubling conserves energy rather than photon number

A lossless idealized frequency doubler converts pairs of input photons at frequency f into single photons at 2f. For a real device, a fraction η=.800\eta=.800 of incident optical power emerges in the doubled-frequency beam; the rest remains at f.

Diagram shown in the original SVG worksheet.

  1. Find doubled-frequency and residual photon rates in terms of input rate Ṅ\dot N.

  2. Find the total output photon rate and verify energy conservation.

Question 6 - Solution

Frequency doubling conserves energy rather than photon number

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2hfṄ2f=ηhfṄ⇒Ṅ2f=.400Ṅ.2hf\dot N_{2f}=\eta hf\dot N\quad\Rightarrow\quad\boxed{\dot N_{2f}=.400\dot N}.hfṄf=(1−η)hfṄ⇒Ṅf=.200Ṅ.hf\dot N_f=(1-\eta)hf\dot N\quad\Rightarrow\quad\boxed{\dot N_f=.200\dot N}.

(b) Interpretation and further calculation

Ṅout=.600Ṅ.\boxed{\dot N_{\mathrm{out}}=.600\dot N}.Pout=hf(.200Ṅ)+2hf(.400Ṅ)=hfṄ=Pin.P_{\mathrm{out}}=hf(.200\dot N)+2hf(.400\dot N)=\boxed{hf\dot N=P_{\mathrm{in}}}.

Physical check

Photon number need not be conserved in a nonlinear optical conversion, while the stated energy accounting must hold.