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 15:00, 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
- E. P. Wigner, Gruppentheorie und ihre Anwendungen auf die Quantenmechanik der Atomspektren, Vieweg Verlag, Braunschweig (1931).