Wigner D-matrix: Difference between revisions

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\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)!} \\
&&\times \left(\cos\frac{\beta}{2}\right)^{2j+m-m'-2s}\left(\sin\frac{\beta}{2}\right)^{m'-m+2s}
&&\times \left(\cos\frac{\beta}{2}\right)^{2j+m-m'-2s}\left(\sin\frac{\beta}{2}\right)^{m'-m+2s}
\end{array}  
\end{array} </math>
</math>
This represents a rotation of <math>\theta</math> about the (inital frame) <math>Y</math> axis.
=== Relation with spherical harmonic functions ===
=== Relation with spherical harmonic functions ===
The D-matrix elements with second index equal to zero, are proportional
The D-matrix elements with second index equal to zero, are proportional

Revision as of 16:00, 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

This represents a rotation of about the (inital frame) axis.

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).