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 14:50, 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
- E. P. Wigner, Gruppentheorie und ihre Anwendungen auf die Quantenmechanik der Atomspektren, Vieweg Verlag, Braunschweig (1931).