Nuclear Models — Question 7

Section 42-8 · Physics pages 7144–7145

Question 7 An unpaired nucleon fixes the simplest shell-model spin and parity An even-even nuclear core has Jπ = 0+. One added neutron occupies an f7/2 orbital, where f means orbital angular momentum ℓ= 3. Use a supplied magnetic factor gj = −.500 and µz = gjµNmj. z x J θ Schematic; labels, not drawing lengths, specify the data. (a) Find total spin-parity and the number of magnetic substates. (b) Find the magnetic moment projection in the stretched state mj = j and distinguish it from the angular-momentum magnitude.
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Question 7 - Solution An unpaired nucleon fixes the simplest shell-model spin and parity z x J θ (a) Method and calculation J = j = 7/2, π = (−1)ℓ= (−1)3 ⇒Jπ = 7/2−. 2J + 1 = 8 magnetic substates . (b) Interpretation and further calculation µz(mj = j) = (−.500)(7/2)µN = −1.75µN . |J| = √ j(j + 1)ℏ= √ 63 2 ℏ̸ = jℏ. Physical check The paired core supplies no net angular momentum in this model. Configuration mixing and collective motion can modify real nuclear moments.

Question 7

An unpaired nucleon fixes the simplest shell-model spin and parity

An even-even nuclear core has Jπ=0+J^\pi=0^+. One added neutron occupies an f7/2f_{7/2} orbital, where f means orbital angular momentum ℓ=3\ell=3. Use a supplied magnetic factor gj=−.500g_j=-.500 and μz=gjμNmj\mu_z=g_j\mu_Nm_j.

Diagram shown in the original SVG worksheet.

  1. Find total spin-parity and the number of magnetic substates.

  2. Find the magnetic moment projection in the stretched state mj=jm_j=j and distinguish it from the angular-momentum magnitude.

Question 7 - Solution

An unpaired nucleon fixes the simplest shell-model spin and parity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

J=j=7/2,π=(−1)ℓ=(−1)3⇒Jπ=7/2−.J=j=7/2,\quad\pi=(-1)^\ell=(-1)^3\Rightarrow\boxed{J^\pi=7/2^-}.2J+1=8 magnetic substates.\boxed{2J+1=8\text{ magnetic substates}}.

(b) Interpretation and further calculation

μz(mj=j)=(−.500)(7/2)μN=−1.75μN.\boxed{\mu_z(m_j=j)=(-.500)(7/2)\mu_N=-1.75\mu_N}.|𝑱|=j(j+1)ℏ=632ℏ≠jℏ.\boxed{|\mathbf J|=\sqrt{j(j+1)}\hbar=\frac{\sqrt{63}}2\hbar\ne j\hbar}.

Physical check

The paired core supplies no net angular momentum in this model. Configuration mixing and collective motion can modify real nuclear moments.