The Eightfold Way — Question 9

Section 44-6 · Physics pages 7408–7409

Question 9 An isospin ladder distinguishes the two central octet states Use dimensionless isospin operators I+|I, m⟩= p I(I + 1) −m(m + 1)|I, m + 1⟩. Sigma zero has I=1,m=0; Lambda has I=0,m=0. Y I3 Σ− Σ0, Λ Σ+ Light-flavor weight diagram: horizontal coordinate I3, vertical coordinate Y = B + S; axis origins are offset for clarity. (a) Apply the raising operator to both states. (b) Find the squared ladder matrix element for Sigma zero, and explain why it is not itself a probability.
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Question 9 - Solution An isospin ladder distinguishes the two central octet states Y I3 Σ− Σ0, Λ Σ+ (a) Method and calculation I+|Σ0⟩= √ 2 |Σ+⟩. I+|Λ⟩= 0 . (b) Interpretation and further calculation |⟨Σ+|I+|Σ0⟩|2 = 2 . P = ⟨f|U(t)|i⟩ 2 ≤1, I+̸ = U(t). Physical check A ladder operator is not a normalized time-evolution operator. Interaction strength and duration are needed to calculate transition probabilities.

Question 9

An isospin ladder distinguishes the two central octet states

Use dimensionless isospin operators I+|I,m⟩=I(I+1)−m(m+1)|I,m+1⟩I_+|I,m\rangle=\sqrt{I(I+1)-m(m+1)}|I,m+1\rangle. Sigma zero has I=1,m=0; Lambda has I=0,m=0.

Diagram shown in the original SVG worksheet.

  1. Apply the raising operator to both states.

  2. Find the squared ladder matrix element for Sigma zero, and explain why it is not itself a probability.

Question 9 - Solution

An isospin ladder distinguishes the two central octet states

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I+|Σ0⟩=2|Σ+⟩.\boxed{I_+|\Sigma^0\rangle=\sqrt2\,|\Sigma^+\rangle}.I+|Λ⟩=0.\boxed{I_+|\Lambda\rangle=0}.

(b) Interpretation and further calculation

|⟨Σ+|I+|Σ0⟩|2=2.\boxed{|\langle\Sigma^+|I_+|\Sigma^0\rangle|^2=2}.P=|⟨f|U(t)|i⟩|2≤1,I+≠U(t).P=\big|\langle f|U(t)|i\rangle\big|^2\le1,\quad I_+\ne U(t).

Physical check

A ladder operator is not a normalized time-evolution operator. Interaction strength and duration are needed to calculate transition probabilities.