An Interlude — Question 1

Section 44-2 · Physics pages 7312–7313

Question 1 Spin projections distinguish state counting from vector magnitude A massive particle has spin quantum number s=3/2. Use Sz = msℏand |S| = √ s(s + 1)ℏ. z x S θ Schematic; labels, not drawing lengths, specify the data. (a) List allowed spin projections and find the number of states. (b) Compare maximum projection with spin magnitude and classify its spin statistics.
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Question 1 - Solution Spin projections distinguish state counting from vector magnitude z x S θ (a) Method and calculation ms = −3/2, −1/2, +1/2, +3/2, g = 2s + 1 = 4 . Sz,max = 3ℏ/2 . (b) Interpretation and further calculation |S| = √ 15ℏ/2 > Sz,max . s ∈Z + 1 2 ⇒fermion; identical particles obey Fermi statistics . Physical check Spin magnitude is not one of its projection eigenvalues. Spatial and other internal quantum numbers also enter the full single-particle state.

Question 1

Spin projections distinguish state counting from vector magnitude

A massive particle has spin quantum number s=3/2. Use Sz=msℏS_z=m_s\hbar and |𝑺|=s(s+1)ℏ|\mathbf S|=\sqrt{s(s+1)}\hbar.

Diagram shown in the original SVG worksheet.

  1. List allowed spin projections and find the number of states.

  2. Compare maximum projection with spin magnitude and classify its spin statistics.

Question 1 - Solution

Spin projections distinguish state counting from vector magnitude

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ms=−3/2,−1/2,+1/2,+3/2,g=2s+1=4.\boxed{m_s=-3/2,-1/2,+1/2,+3/2,\quad g=2s+1=4}.Sz,max=3ℏ/2.\boxed{S_{z,\max}=3\hbar/2}.

(b) Interpretation and further calculation

|𝑺|=15ℏ/2>Sz,max.\boxed{|\mathbf S|=\sqrt{15}\hbar/2>S_{z,\max}}.s∈ℤ+12⇒fermion; identical particles obey Fermi statistics.s\in\mathbb Z+\tfrac12\Rightarrow\boxed{\text{fermion; identical particles obey Fermi statistics}}.

Physical check

Spin magnitude is not one of its projection eigenvalues. Spatial and other internal quantum numbers also enter the full single-particle state.