Principles of Quantum Mechanics · Problem 15.3.3

Addition of Angular Momenta — R. Shankar

Physics — Quantum Mechanics · wigner-eckart-theorem

Problem

(1) Using ⟨jj∣J1∣aj⟩=[j/(j+1)]1/2\langle jj|J_1|aj\rangle = [j/(j+1)]^{1/2} show that ⟨aj∣∣J1∣∣a′j′⟩=δaa′δjj′ℏ[j(j+1)]1/2\langle aj||J_1||a'j'\rangle = \delta_{aa'}\delta_{jj'}\hbar[j(j+1)]^{1/2} (2) Using J⋅A=JzAz+12(J−A++J+A−)\mathbf{J}\cdot\mathbf{A} = J_z A_z + \frac{1}{2}(J_- A_+ + J_+ A_-) (where A±=Ax±iAyA_{\pm} = A_x \pm iA_y) argue that ⟨a′jm′∣J⋅A∣ajm⟩=c⟨a′j∣∣A∣∣aj⟩\langle a'jm'|\mathbf{J}\cdot\mathbf{A}|ajm\rangle = c\langle a'j||A||aj\rangle where cc is a constant independent of aa, a′a' and A\mathbf{A}. Show that c=ℏ[j(j+1)]1/2δm,m′c = \hbar[j(j+1)]^{1/2}\delta_{m,m'}. (3) Using the above, show that ⟨a′jm′∣Aq∣ajm⟩=⟨a′jm∣J⋅A∣ajm⟩ℏ2j(j+1)⟨jm′∣Jq∣jm⟩(15.3.…)\langle a'jm'|A^q|ajm\rangle = \frac{\langle a'jm|\mathbf{J}\cdot\mathbf{A}|ajm\rangle}{\hbar^2 j(j+1)}\langle jm'|J^q|jm\rangle \tag{15.3.\ldots}

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