The Stern-Gerlach Experiment — Question 8

Section 40-4 · Physics pages 6646–6647

Question 8 More than two spots reveal a larger total angular momentum Neutral atoms have J = 3/2 and magnetic projections µz = −gJµBmJ, with gJ = 4/3. A gradient G acts for time t with no drift. Initial transverse velocities vanish and all four sublevels are equally populated. G Schematic; labels, not drawing lengths, specify the data. (a) Find the detector positions after the magnet in terms of K = µBGt2/(2M). (b) Find the adjacent spacing and intensity fraction of each spot.
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Question 8 - Solution More than two spots reveal a larger total angular momentum G (a) Method and calculation z = 1 2(µzG/M)t2 = −gJmJK, mJ = −3/2, −1/2, 1/2, 3/2. z/K = 2, 2/3, −2/3, −2 . (b) Interpretation and further calculation ∆zadj = 4K/3 . Φeach/Φ0 = 1/(2J + 1) = 1/4 . Physical check Number of spots measures available projections when all are populated and resolved. Four spots do not mean four possible electron spin projections; J includes other angular momentum.

Question 8

More than two spots reveal a larger total angular momentum

Neutral atoms have J=3/2J=3/2 and magnetic projections μz=−gJμBmJ\mu_z=-g_J\mu_Bm_J, with gJ=4/3g_J=4/3. A gradient G acts for time t with no drift. Initial transverse velocities vanish and all four sublevels are equally populated.

Diagram shown in the original SVG worksheet.

  1. Find the detector positions after the magnet in terms of K=μBGt2/(2M)K=\mu_BGt^2/(2M).

  2. Find the adjacent spacing and intensity fraction of each spot.

Question 8 - Solution

More than two spots reveal a larger total angular momentum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

z=12(μzG/M)t2=−gJmJK,mJ=−3/2,−1/2,1/2,3/2.z=\tfrac12(\mu_zG/M)t^2=-g_Jm_JK,\quad m_J=-3/2,-1/2,1/2,3/2.z/K=2,2/3,−2/3,−2.\boxed{z/K=2,\ 2/3,\ -2/3,\ -2}.

(b) Interpretation and further calculation

Δzadj=4K/3.\boxed{\Delta z_{\mathrm{adj}}=4K/3}.Φeach/Φ0=1/(2J+1)=1/4.\boxed{\Phi_{\mathrm{each}}/\Phi_0=1/(2J+1)=1/4}.

Physical check

Number of spots measures available projections when all are populated and resolved. Four spots do not mean four possible electron spin projections; J includes other angular momentum.