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Wigner Symbols

Wigner symbols package angular-momentum coupling data. This page fixes the convention and gives selection rules; use a validated generated source for large tables.

Clebsch–Gordan coefficients and Wigner 3-j symbols are related by

⟨j1m1,j2m2∣JM⟩=(−1)j1−j2+M2J+1(j1j2Jm1m2−M).\langle j_1m_1,j_2m_2\vert JM\rangle =(-1)^{j_1-j_2+M}\sqrt{2J+1} \begin{pmatrix} j_1&j_2&J\\ m_1&m_2&-M \end{pmatrix}.

This page uses the Condon–Shortley phase convention.

SymbolRoleTypical Use
3-jrecouples two angular momenta to one totalClebsch–Gordan coefficients, tensor operators
6-jchanges the order of coupling three angular momentarecoupling identities and spin networks
9-jcompares two binary coupling schemes for four angular momentamulti-particle angular momentum
ConditionConsequence
m1+m2+m3=0m_1+m_2+m_3=0otherwise the 3-j symbol vanishes
∣j1−j2∣≤j3≤j1+j2\lvert j_1-j_2\rvert\le j_3\le j_1+j_2triangle condition
j1+j2+j3j_1+j_2+j_3 integerhalf-integer parity consistency
∣mi∣≤ji\lvert m_i\rvert\le j_imagnetic quantum numbers must be valid

Useful special case:

(jj0m−m0)=(−1)j−m2j+1.\begin{pmatrix} j&j&0\\ m&-m&0 \end{pmatrix} =\frac{(-1)^{j-m}}{\sqrt{2j+1}}.
  • Missing the phase factor relating 3-j symbols to Clebsch–Gordan coefficients.
  • Comparing 6-j or 9-j symbols without checking the ordering of entries.
  • Treating selection rules as sufficient for a nonzero value; some allowed entries can still vanish.
  • Copying a table generated with a different phase convention.
  • 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.
  • D. M. Brink and G. R. Satchler, Angular Momentum, 3rd ed., Oxford University Press, 1993.