6-j symbol

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Wigner's 6 − j symbols were introduced by Eugene Paul Wigner in 1940, and published in 1965. They are related to Racah's W-coefficients by


  \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6
  \end{Bmatrix}
   = (-1)^{j_1+j_2+j_4+j_5}W(j_1j_2j_5j_4;j_3j_6).

They have higher symmetry than Racah's W-coefficients.

Contents

[edit] Symmetry relations

The 6 − j symbol is invariant under the permutation of any two columns:


 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6
 \end{Bmatrix}
 =
 \begin{Bmatrix}
    j_2 & j_1 & j_3\\
    j_5 & j_4 & j_6
 \end{Bmatrix}
=
 \begin{Bmatrix}
    j_1 & j_3 & j_2\\
    j_4 & j_6 & j_5
 \end{Bmatrix}
=
 \begin{Bmatrix}
    j_3 & j_2 & j_1\\
    j_6 & j_5 & j_4
 \end{Bmatrix}.

The 6 − j symbol is also invariant if upper and lower arguments are interchanged in any two columns:


 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6
 \end{Bmatrix}
 =
 \begin{Bmatrix}
    j_4 & j_5 & j_3\\
    j_1 & j_2 & j_6
 \end{Bmatrix}
 =
 \begin{Bmatrix}
    j_1 & j_5 & j_6\\
    j_4 & j_2 & j_3
 \end{Bmatrix}
 =
 \begin{Bmatrix}
    j_4 & j_2 & j_6\\
    j_1 & j_5 & j_3
 \end{Bmatrix}.

The 6 − j symbol


 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6
 \end{Bmatrix}

is zero unless j1, j2, and j3 satisfy triangle conditions, i.e.,


  j_1 = |j_2-j_3|, \ldots, j_2+j_3.

In combination with the symmetry relation for interchanging upper and lower arguments this shows that triangle conditions must also be satisfied for (j1,j5,j6), (j4,j2,j6), and (j4,j5,j3).

[edit] Special case

When j6 = 0 the expression for the 6-j symbol is:


 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & 0
 \end{Bmatrix}
 = \frac{\delta_{j_2,j_4}\delta_{j_1,j_5}}{\sqrt{(2j_1+1)(2j_2+1)}} (-1)^{j_1+j_2+j_3}\Delta(j_1,j_2,j_3).

The function Δ(j1,j2,j3) is equal to 1 when (j1,j2,j3) satisfy the triangle conditions, and zero otherwise. The symmetry relations can be used to find the expression when another j is equal to zero.

[edit] Orthogonality relation

The 6-j symbols satisfy this orthogonality relation:


  \sum_{j_3} (2j_3+1)
 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6
 \end{Bmatrix}
 \begin{Bmatrix}
    j_1 & j_2 & j_3\\
    j_4 & j_5 & j_6'
 \end{Bmatrix}
  = \frac{\delta_{j_6^{}j_6'}}{2j_6+1} \Delta(j_1,j_5,j_6) \Delta(j_4,j_2,j_6).

[edit] See also

[edit] External links

[edit] References

  • Biedenharn, L. C.; van Dam, H. (1965). Quantum Theory of Angular Momentum: A collection of Reprints and Original Papers. New York: Academic Press. ISBN 0120960567.