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 2j+1, given by

Dm′mj(α,β,γ):=⟨jm′|R(α,β,γ)|jm⟩=e−im′αdm′mj(β)e−imγ

where α,β, and γ are Euler angles, and where dm′mj(β), known as Wigner's reduced d-matrix, is given by

dm′mj(β)=Dm′mj(0,β,0)=⟨jm'|e−iβjy|jm⟩=[(j+m')!(j−m')!(j+m)!(j−m)!]1/2∑s(−1)m′−m+s(j+m−s)!s!(m′−m+s)!(j−m′−s)!×(cosβ2)2j+m−m′−2s(sinβ2)m′−m+2s

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

Relation with spherical harmonic functions

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

Dm0ℓ(α,β,γ)*=4π2ℓ+1Yℓm(β,α)

External links

References

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