Angular Momenta and Magnetic Dipole Moments — Question 7

Section 40-3 · Physics pages 6624–6625

Question 7 A Lande factor connects weak-field splitting to coupled angular momentum For gL = 1 and gs = 2, use gJ = 1 + [j(j + 1) + s(s + 1) −l(l + 1)]/[2j(j + 1)]. A p electron has l = 1, s = 1/2. In a weak field, δE = gJµBBmj. j = 1/2 j = 3/2 ∆E Schematic; labels, not drawing lengths, specify the data. (a) Calculate the two Lande factors. (b) Find the ratio of adjacent Zeeman spacings in the j = 3/2 and j = 1/2 multiplets.
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Question 7 - Solution A Lande factor connects weak-field splitting to coupled angular momentum j = 1/2 j = 3/2 ∆E (a) Method and calculation g3/2 = 1 + 15/4 + 3/4 −2 2(15/4) = 4/3 . g1/2 = 1 + 3/4 + 3/4 −2 2(3/4) = 2/3 . (b) Interpretation and further calculation ∆Ej = gJµBB (∆mj = 1). ∆E3/2/∆E1/2 = (4/3)/(2/3) = 2 . Physical check The field must be weak relative to the spin-orbit splitting so that j remains a useful label. These factors are effective projections of orbital and spin moments onto total J.

Question 7

A Lande factor connects weak-field splitting to coupled angular momentum

For gL=1g_L=1 and gs=2g_s=2, use gJ=1+[j(j+1)+s(s+1)−l(l+1)]/[2j(j+1)]g_J=1+[j(j+1)+s(s+1)-l(l+1)]/[2j(j+1)]. A p electron has l=1,s=1/2l=1,s=1/2. In a weak field, δE=gJμBBmj\delta E=g_J\mu_BBm_j.

Diagram shown in the original SVG worksheet.

  1. Calculate the two Lande factors.

  2. Find the ratio of adjacent Zeeman spacings in the j=3/2j=3/2 and j=1/2j=1/2 multiplets.

Question 7 - Solution

A Lande factor connects weak-field splitting to coupled angular momentum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

g3/2=1+15/4+3/4−22(15/4)=4/3.g_{3/2}=1+\frac{15/4+3/4-2}{2(15/4)}=\boxed{4/3}.g1/2=1+3/4+3/4−22(3/4)=2/3.g_{1/2}=1+\frac{3/4+3/4-2}{2(3/4)}=\boxed{2/3}.

(b) Interpretation and further calculation

ΔEj=gJμBB(Δmj=1).\Delta E_j=g_J\mu_BB\quad(\Delta m_j=1).ΔE3/2/ΔE1/2=(4/3)/(2/3)=2.\boxed{\Delta E_{3/2}/\Delta E_{1/2}=(4/3)/(2/3)=2}.

Physical check

The field must be weak relative to the spin-orbit splitting so that j remains a useful label. These factors are effective projections of orbital and spin moments onto total J.