Wigner D-matrix: Difference between revisions

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:<math>\begin{array}{lcl}
:<math>\begin{array}{lcl}
d^j_{m'm}(\beta) &=& \langle jm' |e^{-i\beta j_y} | jm \rangle\\
d^j_{m'm}(\beta) &=& D^j_{m'm}(0,\beta,0) \\
&=& \langle jm' |e^{-i\beta j_y} | jm \rangle\\
&=& [(j+m')!(j-m')!(j+m)!(j-m)!]^{1/2}
&=& [(j+m')!(j-m')!(j+m)!(j-m)!]^{1/2}
\sum_s \frac{(-1)^{m'-m+s}}{(j+m-s)!s!(m'-m+s)!(j-m'-s)!} \\
\sum_s \frac{(-1)^{m'-m+s}}{(j+m-s)!s!(m'-m+s)!(j-m'-s)!} \\

Revision as of 15:50, 17 June 2008

The Wigner D-matrix is a square matrix, of dimension , given by

where and are Euler angles, and where , known as Wigner's reduced d-matrix, is given by

Relation with spherical harmonic functions

The D-matrix elements with second index equal to zero, are proportional to spherical harmonics (normalized to unity)

External links

References

  1. E. P. Wigner, Gruppentheorie und ihre Anwendungen auf die Quantenmechanik der Atomspektren, Vieweg Verlag, Braunschweig (1931).