How Lasers Work — Question 2

Section 40-11 · Physics pages 6774–6775

Question 2 Steady resonant pumping cannot invert an ideal two-level atom An equal-degeneracy two-level ensemble has total population N. Resonant incoherent light drives upward and downward stimulated transitions at rate W per atom, and spontaneous decay has rate A. Use ˙N2 = WN1 −WN2 −AN2. lower upper ∆E Schematic; labels, not drawing lengths, specify the data. (a) Find the steady upper-level fraction. (b) Find the steady population difference and its limit as W →∞.
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Question 2 - Solution Steady resonant pumping cannot invert an ideal two-level atom lower upper ∆E (a) Method and calculation N1 = N −N2 : 0 = WN −(2W + A)N2. N2/N = W/(2W + A) < 1/2 (A > 0). (b) Interpretation and further calculation (N2 −N1)/N = 2W/(2W + A) −1 = −A/(2W + A) . W →∞: N2/N →1/2, N2 −N1 →0−. Physical check This impossibility result concerns steady incoherent resonant pumping in the stated closed two-level model. A coherent pi pulse can transiently invert a two-level system and is a different preparation.

Question 2

Steady resonant pumping cannot invert an ideal two-level atom

An equal-degeneracy two-level ensemble has total population N. Resonant incoherent light drives upward and downward stimulated transitions at rate W per atom, and spontaneous decay has rate A. Use Ṅ2=WN1−WN2−AN2\dot N_2=WN_1-WN_2-AN_2.

Diagram shown in the original SVG worksheet.

  1. Find the steady upper-level fraction.

  2. Find the steady population difference and its limit as W→∞W\to\infty.

Question 2 - Solution

Steady resonant pumping cannot invert an ideal two-level atom

Diagram shown in the original SVG worksheet.

(a) Method and calculation

N1=N−N2:0=WN−(2W+A)N2.N_1=N-N_2:\quad0=WN-(2W+A)N_2.N2/N=W/(2W+A)<1/2(A>0).\boxed{N_2/N=W/(2W+A)<1/2}\quad(A>0).

(b) Interpretation and further calculation

(N2−N1)/N=2W/(2W+A)−1=−A/(2W+A).\boxed{(N_2-N_1)/N=2W/(2W+A)-1=-A/(2W+A)}.W→∞:N2/N→1/2,N2−N1→0−.W\to\infty:\quad\boxed{N_2/N\to1/2,\quad N_2-N_1\to0^-}.

Physical check

This impossibility result concerns steady incoherent resonant pumping in the stated closed two-level model. A coherent pi pulse can transiently invert a two-level system and is a different preparation.