A rank-1 (vector) tensor operator connects the and multiplets of a fine-structure doublet

PHYSICS · Subjective · Fermi University Physics · Quantum Mechanics · Symmetry, angular momentum and spin · Symmetry, angular momentum and spin

The Structure of Quantum Mechanics, Ch Adding angular momenta, tensor operators and Wigner-Eckart

Problem

A rank-1 (vector) tensor operator V^q(1)\hat V^{(1)}_q connects the j=32j=\tfrac32 and j=12j=\tfrac12 multiplets of a fine-structure doublet. Its reduced matrix element is ⟨32 ∥V^(1)∥ 12⟩=6.0×10−2 ea0\langle \tfrac32\,\|\hat V^{(1)}\|\,\tfrac12\rangle = 6.0\times10^{-2}\,e a_0, where ee is the electron charge and a0a_0 the Bohr radius.Using the Wigner-Eckart theorem in the form ⟨j′,m′∣T^q∣j,m⟩=⟨j,m;k,q∣j′,m′⟩ ⟨j′∥T^∥j⟩/2j′+1\langle j',m'|\hat T_q|j,m\rangle=\langle j,m;k,q|j',m'\rangle\,\langle j'\|\hat T\|j\rangle/\sqrt{2j'+1} and the Clebsch-Gordan coefficient ⟨12,12;1,0 ∣ 32,12⟩=2/3\langle \tfrac12,\tfrac12;1,0\,|\,\tfrac32,\tfrac12\rangle=\sqrt{2/3} (built from the ladder construction for 1⊗121\otimes\tfrac12), find ⟨32,12∣V^0(1)∣12,12⟩\langle \tfrac32,\tfrac12|\hat V^{(1)}_0|\tfrac12,\tfrac12\rangle.

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