Angular Momenta and Magnetic Dipole Moments โ€” Question 6

Section 40-3 ยท Physics pages 6622โ€“6623

Question 6 Spin-orbit energies follow from the square of total angular momentum Use Hso = AL ยท S/โ„2 with A > 0. A p electron has l = 1, s = 1/2 and total J = L + S. j = 1/2 j = 3/2 โˆ†E Schematic; labels, not drawing lengths, specify the data. (a) Derive the energy for each allowed j. (b) Find the splitting and the degeneracy-weighted mean energy.
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Question 6 - Solution Spin-orbit energies follow from the square of total angular momentum j = 1/2 j = 3/2 โˆ†E (a) Method and calculation 2L ยท S = J2 โˆ’L2 โˆ’S2 โ‡’Ej = A 2 [j(j + 1) โˆ’2 โˆ’3/4]. E3/2 = A/2, E1/2 = โˆ’A . (b) Interpretation and further calculation E3/2 โˆ’E1/2 = 3A/2 . ยฏE = 4(A/2) + 2(โˆ’A) 6 = 0 . Physical check The weighted centroid remains at the unsplit energy in this model. Reversing the sign of A reverses the level ordering.

Question 6

Spin-orbit energies follow from the square of total angular momentum

Use Hso=A๐‘ณโ‹…๐‘บ/โ„2H_{\mathrm{so}}=A\boldsymbol L\cdot\boldsymbol S/\hbar^2 with A>0A>0. A p electron has l=1,s=1/2l=1,s=1/2 and total ๐‘ฑ=๐‘ณ+๐‘บ\boldsymbol J=\boldsymbol L+\boldsymbol S.

Diagram shown in the original SVG worksheet.

  1. Derive the energy for each allowed j.

  2. Find the splitting and the degeneracy-weighted mean energy.

Question 6 - Solution

Spin-orbit energies follow from the square of total angular momentum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2๐‘ณโ‹…๐‘บ=J2โˆ’L2โˆ’S2โ‡’Ej=A2[j(j+1)โˆ’2โˆ’3/4].2\boldsymbol L\cdot\boldsymbol S=J^2-L^2-S^2\Rightarrow E_j=\tfrac A2[j(j+1)-2-3/4].E3/2=A/2,E1/2=โˆ’A.\boxed{E_{3/2}=A/2,\quad E_{1/2}=-A}.

(b) Interpretation and further calculation

E3/2โˆ’E1/2=3A/2.\boxed{E_{3/2}-E_{1/2}=3A/2}.Eโ€พ=4(A/2)+2(โˆ’A)6=0.\bar E=\frac{4(A/2)+2(-A)}{6}=\boxed{0}.

Physical check

The weighted centroid remains at the unsplit energy in this model. Reversing the sign of A reverses the level ordering.