Angular Momenta and Magnetic Dipole Moments — Question 8

Section 40-3 · Physics pages 6626–6627

Question 8 A strong field reveals coincident shifts from different spin-orbital states In a field strong enough to neglect spin-orbit coupling, a p electron has ml = −1, 0, 1 and ms = ±1/2. Use δE = µBB(ml + 2ms) and omit quadratic magnetic terms. −2µBB −1µBB 0µBB 1µBB 2µBB g = 2 Schematic; labels, not drawing lengths, specify the data. (a) Find the distinct shift values and their multiplicities. (b) Calculate the mean and variance of the energy shift for equal population of the six states.
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Question 8 - Solution A strong field reveals coincident shifts from different spin-orbital states −2µBB −1µBB 0µBB 1µBB 2µBB g = 2 (a) Method and calculation ms = +1/2 : (0, 1, 2)µBB; ms = −1/2 : (−2, −1, 0)µBB. δE/µBB = −2, −1, 0, 1, 2; g = 1, 1, 2, 1, 1 . (b) Interpretation and further calculation ⟨δE⟩= (−2 −1 + 0 + 0 + 1 + 2)µBB 6 = 0 . Var(δE) = 4 + 1 + 0 + 0 + 1 + 4 6 (µBB)2 = 5 3(µBB)2 . Physical check Six basis states produce only five distinct shifts because two states coincide at zero. Multiplicity must be retained in averages.

Question 8

A strong field reveals coincident shifts from different spin-orbital states

In a field strong enough to neglect spin-orbit coupling, a p electron has ml=−1,0,1m_l=-1,0,1 and ms=±1/2m_s=\pm1/2. Use δE=μBB(ml+2ms)\delta E=\mu_BB(m_l+2m_s) and omit quadratic magnetic terms.

Diagram shown in the original SVG worksheet.

  1. Find the distinct shift values and their multiplicities.

  2. Calculate the mean and variance of the energy shift for equal population of the six states.

Question 8 - Solution

A strong field reveals coincident shifts from different spin-orbital states

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ms=+1/2:(0,1,2)μBB;ms=−1/2:(−2,−1,0)μBB.m_s=+1/2:\ (0,1,2)\mu_BB;\qquad m_s=-1/2:\ (-2,-1,0)\mu_BB.δE/μBB=−2,−1,0,1,2;g=1,1,2,1,1.\boxed{\delta E/\mu_BB=-2,-1,0,1,2;\quad g=1,1,2,1,1}.

(b) Interpretation and further calculation

⟨δE⟩=(−2−1+0+0+1+2)μBB6=0.\langle\delta E\rangle=\frac{(-2-1+0+0+1+2)\mu_BB}{6}=\boxed{0}.Var(δE)=4+1+0+0+1+46(μBB)2=53(μBB)2.\boxed{\mathrm{Var}(\delta E)=\frac{4+1+0+0+1+4}{6}(\mu_BB)^2=\frac53(\mu_BB)^2}.

Physical check

Six basis states produce only five distinct shifts because two states coincide at zero. Multiplicity must be retained in averages.