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Wigner–Eckart Theorem

For a spherical tensor operator Tq(k)T_q^{(k)}, rotational symmetry factors angular-momentum matrix elements into a known angular coefficient and a reduced matrix element independent of magnetic quantum numbers.

With the convention used in the formula card,

⟨j′m′∣Tq(k)∣jm⟩=(−1)j′−m′(j′kj−m′qm)⟨j′∥T(k)∥j⟩.\langle j' m'\vert T^{(k)}_q\vert j m\rangle = (-1)^{j'-m'} \begin{pmatrix} j'&k&j\\ -m'&q&m \end{pmatrix} \langle j'\lVert T^{(k)}\rVert j\rangle.

The angular coefficient enforces

m′=m+q,∣j−k∣≤j′≤j+k.m'=m+q, \qquad \lvert j-k\rvert\le j'\le j+k.

Other symmetries, such as parity or exchange symmetry, can add further selection rules.

  • The states transform as angular-momentum eigenstates under the same SU(2)SU(2) convention.
  • Tq(k)T_q^{(k)} is a spherical tensor operator of rank kk.
  • Clebsch-Gordan and Wigner 3j3j phase conventions are used consistently.
  • The reduced-matrix-element normalization matches the chosen convention.

The theorem says that symmetry controls the dependence on m,m′,qm,m',q. Dynamics and radial or internal structure are contained in the reduced matrix element. This is why large families of transition amplitudes can be related before doing detailed integrals.

  • Mixing reduced-matrix-element conventions from different books.
  • Treating the reduced matrix element as fixed by symmetry alone.
  • Forgetting that parity and other discrete symmetries supply additional rules.
  • Applying the theorem to an operator that is not a spherical tensor.
  • Losing phase signs by switching between 3j3j and Clebsch-Gordan conventions.

What does the theorem say for a scalar operator with k=0k=0?

Solution

Only q=0q=0 exists. The selection rules give m′=mm'=m and j′=jj'=j. A rotational scalar is diagonal in jj and mm, up to any additional degeneracy labels not shown.

  • E. P. Wigner, Group Theory and Its Application to the Quantum Mechanics of Atomic Spectra, Academic Press, 1959.
  • A. R. Edmonds, Angular Momentum in Quantum Mechanics, Princeton University Press, 1957.
  • D. A. Varshalovich, A. N. Moskalev, and V. K. Khersonskii, Quantum Theory of Angular Momentum, World Scientific, 1988.
  • J. J. Sakurai and J. Napolitano, Modern Quantum Mechanics, 3rd ed., Cambridge University Press, 2020.