Wigner_D-matrix

Wigner D-matrix

The Wigner D-matrix is a matrix in an irreducible representation of the groups SU(2) and SO(3). The complex conjugate of the D-matrix is an eigenfunction of the Hamiltonian of spherical and symmetric rigid rotors. The matrix was introduced in 1927 by Eugene Wigner.

1 Definition Wigner D-matrix
2 Wigner (small) d-matrix
3 Properties of Wigner D-matrix
4 Orthogonality relations
5 Relation with spherical harmonic functions
6 Relation with Legendre polynomials
7 Relation to Bessel Function
8 Table of d-matrix Elements
9 See also
10 References
11 External Links

Definition Wigner D-matrix

Let $j x$ , $j y$ , $j z$ be generators of the Lie algebra of SU(2) and SO(3). In quantum mechanics these three operators are the components of a vector operator known as angular momentum. Examples are the angular momentum of an electron in an atom, electronic spin,and the angular momentum of a rigid rotor. In all cases the three operators satisfy the following commutation relations,

$[j_x,j_y] = i j_z,\quad [j_z,j_x] = i j_y,\quad [j_y,j_z] = i j_x,$

where i is the purely imaginary number and Planck's constant $\hbar$ has been put equal to one. The operator

$j^2 = j_x^2 + j_y^2 + j_z^2$

is a Casimir operator of SU(2) (or SO(3) as the case may be). It may be diagonalized together with $j z$ (the choice of this operator is a convention), which commutes with $j 2$ . That is, it can be shown that there is a complete set of kets with

$j^2 |jm\rangle = j(j+1) |jm\rangle,\quad j_z |jm\rangle = m |jm\rangle,$

where $j=0, \tfrac{1}{2}, 1, \tfrac{3}{2}, 2, \dots$ and $m=-j, -j+1, \ldots, j$ . (For SO(3) the quantum number $j$ is integer.)

A rotation operator can be written as

$\mathcal{R}(\alpha,\beta,\gamma) = e^{-i\alpha j_z}e^{-i\beta j_y}e^{-i\gamma j_z},$

where $\alpha, \; \beta,$ and $\gamma\;$ are Euler angles (characterized by the keywords: z-y-z convention, right-handed frame, right-hand screw rule, active interpretation).

The Wigner D-matrix is a square matrix of dimension $2 j + 1$ with general element

$D^j_{m'm}(\alpha,\beta,\gamma) \equiv \langle jm' | \mathcal{R}(\alpha,\beta,\gamma)| jm \rangle = e^{-im'\alpha } d^j_{m'm}(\beta)e^{-i m\gamma}.$

The matrix with general element

$d^j_{m'm}(\beta)= \langle jm' |e^{-i\beta j_y} | jm \rangle$

is known as Wigner's (small) d-matrix.

Wigner (small) d-matrix

Wigner¹ gave the following expression

$\begin{array}{lcl} d^j_{m'm}(\beta) &=& [(j+m')!(j-m')!(j+m)!(j-m)!]^{1/2} \sum_s \frac{(-1)^{m'-m+s}}{(j+m-s)!s!(m'-m+s)!(j-m'-s)!} \\ &&\times \left(\cos\frac{\beta}{2}\right)^{2j+m-m'-2s}\left(\sin\frac{\beta}{2}\right)^{m'-m+2s}. \end{array}$

The sum over s is over such values that the factorials are nonnegative.

Note: The d-matrix elements defined here are real. In the often-used z-x-z convention of Euler angles, the factor $( - 1) m' - m + s$ in this formula is replaced by $(-1)^s\, i^{m-m'}$ , causing half of the functions to be purely imaginary. The realness of the d-matrix elements is one of the reasons that the z-y-z convention, used in this article, is usually preferred in quantum mechanical applications.

The d-matrix elements are related to Jacobi polynomials $P^{(a,b)}_k(\cos\beta)$ with nonnegative $a\,$ and $b\,$ . ² Let

$k = \min(j+m,\,j-m,\,j+m',\,j-m').$

$\hbox{If}\quad k = \begin{cases} j+m: &\quad a=m'-m;\quad \lambda=m'-m\\ j-m: &\quad a=m-m';\quad \lambda= 0 \\ j+m': &\quad a=m-m';\quad \lambda= 0 \\ j-m': &\quad a=m'-m;\quad \lambda=m'-m \\ \end{cases}$

Then, with $b=2j-2k-a\,$ , the relation is

$d^j_{m'm}(\beta) = (-1)^{\lambda} \binom{2j-k}{k+a}^{1/2} \binom{k+b}{b}^{-1/2} \left(\sin\frac{\beta}{2}\right)^a \left(\cos\frac{\beta}{2}\right)^b P^{(a,b)}_k(\cos\beta),$

where $a,b \ge 0. \,$

Properties of Wigner D-matrix

The complex conjugate of the D-matrix satisfies a number of differential properties that can be formulated concisely by introducing the following operators with $(x,\, y,\,z) = (1,\,2,\,3)$ ,

$\begin{array}{lcl} \hat{\mathcal{J}}_1 &=& i \left( \cos \alpha \cot \beta \, {\partial \over \partial \alpha} \, + \sin \alpha \, {\partial \over \partial \beta} \, - {\cos \alpha \over \sin \beta} \, {\partial \over \partial \gamma} \, \right) \\ \hat{\mathcal{J}}_2 &=& i \left( \sin \alpha \cot \beta \, {\partial \over \partial \alpha} \, - \cos \alpha \; {\partial \over \partial \beta } \, - {\sin \alpha \over \sin \beta} \, {\partial \over \partial \gamma } \, \right) \\ \hat{\mathcal{J}}_3 &=& - i \; {\partial \over \partial \alpha} , \end{array}$

which have quantum mechanical meaning: they are space-fixed rigid rotor angular momentum operators.

Further,

$\begin{array}{lcl} \hat{\mathcal{P}}_1 &=& \, i \left( {\cos \gamma \over \sin \beta} {\partial \over \partial \alpha } - \sin \gamma {\partial \over \partial \beta } - \cot \beta \cos \gamma {\partial \over \partial \gamma} \right) \\ \hat{\mathcal{P}}_2 &=& \, i \left( - {\sin \gamma \over \sin \beta} {\partial \over \partial \alpha} - \cos \gamma {\partial \over \partial \beta} + \cot \beta \sin \gamma {\partial \over \partial \gamma} \right) \\ \hat{\mathcal{P}}_3 &=& - i {\partial\over \partial \gamma}, \\ \end{array}$

which have quantum mechanical meaning: they are body-fixed rigid rotor angular momentum operators.

The operators satisfy the commutation relations

$\left[\mathcal{J}_1, \, \mathcal{J}_2\right] = i \mathcal{J}_3, \qquad \hbox{and}\qquad \left[\mathcal{P}_1, \, \mathcal{P}_2\right] = -i \mathcal{P}_3$

and the corresponding relations with the indices permuted cyclically. The $\mathcal{P}_i$ satisfy anomalous commutation relations (have a minus sign on the right hand side).

The two sets mutually commute,

$\left[\mathcal{P}_i, \, \mathcal{J}_j\right] = 0,\quad i,\,j = 1,\,2,\,3,$

and the total operators squared are equal,

$\mathcal{J}^2 \equiv \mathcal{J}_1^2+ \mathcal{J}_2^2 + \mathcal{J}_3^2 = \mathcal{P}^2 \equiv \mathcal{P}_1^2+ \mathcal{P}_2^2 + \mathcal{P}_3^2 .$

Their explicit form is,

$\mathcal{J}^2= \mathcal{P}^2 = -\frac{1}{\sin^2\beta} \left( \frac{\partial^2}{\partial \alpha^2} +\frac{\partial^2}{\partial \gamma^2} -2\cos\beta\frac{\partial^2}{\partial\alpha\partial \gamma} \right) -\frac{\partial^2}{\partial \beta^2} -\cot\beta\frac{\partial}{\partial \beta}.$

The operators $\mathcal{J}_i$ act on the first (row) index of the D-matrix,

$\mathcal{J}_3 \, D^j_{m'm}(\alpha,\beta,\gamma)^* = m' \, D^j_{m'm}(\alpha,\beta,\gamma)^* ,$

and

$(\mathcal{J}_1 \pm i \mathcal{J}_2)\, D^j_{m'm}(\alpha,\beta,\gamma)^* = \sqrt{j(j+1)-m'(m'\pm 1)} \, D^j_{m'\pm 1, m}(\alpha,\beta,\gamma)^* .$

The operators $\mathcal{P}_i$ act on the second (column) index of the D-matrix

$\mathcal{P}_3 \, D^j_{m'm}(\alpha,\beta,\gamma)^* = m \, D^j_{m'm}(\alpha,\beta,\gamma)^* ,$

and because of the anomalous commutation relation the raising/lowering operators are defined with reversed signs,

$(\mathcal{P}_1 \mp i \mathcal{P}_2)\, D^j_{m'm}(\alpha,\beta,\gamma)^* = \sqrt{j(j+1)-m(m\pm 1)} \, D^j_{m', m\pm1}(\alpha,\beta,\gamma)^* .$

Finally,

$\mathcal{J}^2\, D^j_{m'm}(\alpha,\beta,\gamma)^* = \mathcal{P}^2\, D^j_{m'm}(\alpha,\beta,\gamma)^* = j(j+1) D^j_{m'm}(\alpha,\beta,\gamma)^*.$

In other words, the rows and columns of the (complex conjugate) Wigner D-matrix span irreducible representations of the isomorphic Lie algebra's generated by $\{\mathcal{J}_i\}$ and $\{-\mathcal{P}_i\}$ .

An important property of the Wigner D-matrix follows from the commutation of $\mathcal{R}(\alpha,\beta,\gamma)$ with the time reversal operator $T\,$ ,

$\langle jm' | \mathcal{R}(\alpha,\beta,\gamma)| jm \rangle = \langle jm' | T^{\,\dagger} \mathcal{R}(\alpha,\beta,\gamma) T| jm \rangle = (-1)^{m'-m} \langle j,-m' | \mathcal{R}(\alpha,\beta,\gamma)| j,-m \rangle^*,$

$D^j_{m'm}(\alpha,\beta,\gamma) = (-1)^{m'-m} D^j_{-m',-m}(\alpha,\beta,\gamma)^*.$

Here we used that $T\,$ is anti-unitary (hence the complex conjugation after moving $T^\dagger\,$ from ket to bra), $T | jm \rangle = (-1)^{j-m} | j,-m \rangle$ and $( - 1) 2 j - m' - m = ( - 1) m' - m$ .

Orthogonality relations

The Wigner D-matrix elements $D^j_{mk}(\alpha,\beta,\gamma)$ form a complete set of orthogonal functions of the Euler angles $α$ , $β,$ and $γ$ :

$\int_0^{2\pi} d\alpha \int_0^\pi \sin \beta d\beta \int_0^{2\pi} d\gamma \,\, D^{j'}_{m'k'}(\alpha,\beta,\gamma)^\ast D^j_{mk}(\alpha,\beta,\gamma) = \frac{8\pi^2}{2j+1} \delta_{m'm}\delta_{k'k}\delta_{j'j}.$

This is a special case of the Schur orthogonality relations.

Relation with spherical harmonic functions

The D-matrix elements with second index equal to zero, are proportional to spherical harmonics, normalized to unity and with Condon and Shortley phase convention,

$D^{\ell}_{m 0}(\alpha,\beta,\gamma)^* = \sqrt{\frac{4\pi}{2\ell+1}} Y_{\ell}^m (\beta, \alpha ) .$

In the present convention of Euler angles, $α$ is a longitudinal angle and $β$ is a colatitudinal angle (spherical polar angles in the physical definition of such angles). This is one of the reasons that the z-y-z convention is used frequently in molecular physics. From the time-reversal property of the Wigner D-matrix follows immediately

$\left( Y_{\ell}^m \right) ^* = (-1)^m Y_{\ell}^{-m}.$

There exists a more general relationship to the spin-weighted spherical harmonics:

$D^{\ell}_{-m s}(\alpha,\beta,-\gamma) =(-1)^m \sqrt\frac{4\pi}{2{\ell}+1} {}_sY_{{\ell}m}(\beta,\alpha) e^{is\gamma}.$

Relation with Legendre polynomials

The Wigner small d-matrix elements with both indices set to zero are related to Legendre polynomials

$d^{\ell}_{0,0}(\beta) = P_{\ell}(\cos\beta).$

Relation to Bessel Function

In the limit when $\ell \gg m, m^\prime$ we have $D^\ell_{mm^\prime}(\alpha,\beta,\gamma) \approx e^{-im\alpha-im^\prime\gamma}J_{m-m^\prime}(\ell\beta)$ where $J_{m-m^\prime}(\ell\beta)$ is the Bessel function and $\ell\beta$ is finite.

Table of d-matrix Elements

Using sign convention of Wigner, et. al. the d-matrix elements for j=1/2, 1, 3/2, and 2 are given below.

for j=1/2

$d_{1/2,1/2}^{1/2} = \cos (\theta/2)$
$d_{1/2,-1/2}^{1/2} = -\sin (\theta/2)$

for j=1

$d_{1,1}^{1} = \frac{1+\cos \theta}{2}$
$d_{1,0}^{1} = \frac{-\sin \theta}{\sqrt{2}}$
$d_{1,-1}^{1} = \frac{1-\cos \theta}{2}$
$d_{0,0}^{1} = \cos \theta$

for j=3/2

$d_{3/2,3/2}^{3/2} = \frac{1+\cos \theta}{2} \cos \frac{\theta}{2}$
$d_{3/2,1/2}^{3/2} = -\sqrt{3} \frac{1+\cos \theta}{2} \sin \frac{\theta}{2}$
$d_{3/2,-1/2}^{3/2} = \sqrt{3} \frac{1-\cos \theta}{2} \cos \frac{\theta}{2}$
$d_{3/2,-3/2}^{3/2} = - \frac{1-\cos \theta}{2} \sin \frac{\theta}{2}$
$d_{1/2,1/2}^{3/2} = \frac{3\cos \theta - 1}{2} \cos \frac{\theta}{2}$
$d_{1/2,-1/2}^{3/2} = - \frac{3\cos \theta + 1}{2} \sin \frac{\theta}{2}$

for j=2

$d_{2,2}^{2} = \left(\frac{1+\cos \theta}{2}\right)^2$
$d_{2,1}^{2} = - \frac{1 + \cos \theta}{2} \sin \theta$
$d_{2,0}^{2} = \frac{\sqrt{6}}{4} \sin^2 \theta$
$d_{2,-1}^{2} = - \frac{1 - \cos \theta}{2} \sin \theta$
$d_{2,-2}^{2} = \left(\frac{1-\cos \theta}{2}\right)^2$
$d_{1,1}^{2} = \frac{1+\cos \theta}{2} (2 \cos \theta - 1)$
$d_{1,0}^{2} = -\sqrt{\frac{3}{2}} \sin \theta \cos \theta$
$d_{1,-1}^{2} = \frac{1-\cos \theta}{2} (2 \cos \theta + 1)$
$d_{0,0}^{2} = \frac{3 \cos^2 \theta - 1}{2}$

Wigner d-matrix elements with swapped lower indices are found with the relation: $d_{m', m}^j = (-1)^{m-m'}d_{m, m'}^j$ .

References

Cited references

^ E. P. Wigner, Gruppentheorie und ihre Anwendungen auf die Quantenmechanik der Atomspektren, Vieweg Verlag, Braunschweig (1931). Translated into English: J. J. Griffin, Group Theory and its Application to the Quantum Mechanics of Atomic Spectra, Academic Press, New York (1959).
^ L. C. Biedenharn and J. D. Louck, Angular Momentum in Quantum Physics, Addison-Wesley, Reading, (1981).

External Links

PDG Table of Clebsch-Gordon Coefficients, Spherical Harmonics, and d-Functions

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