The \bgroup\color{black}$\ell=1$\egroup Angular Momentum Operators*

We will use states of definite \bgroup\color{black}$L_z$\egroup, the \bgroup\color{black}$Y_{1m}$\egroup.

\begin{eqnarray*}
& \langle \ell m'\vert L_z\vert\ell m\rangle =m\hbar \delta_{m'm} \\
& L_z=\hbar\left(\matrix{1&0&0\cr 0&0&0\cr 0&0&-1}\right)
\end{eqnarray*}


\begin{eqnarray*}
\langle \ell m'\vert L_\pm\vert\ell m\rangle &=&\sqrt{\ell (\...
...hbar\left(\matrix{0&0&0\cr \sqrt{2}&0&0\cr 0&\sqrt{2}&0}\right)
\end{eqnarray*}


\begin{eqnarray*}
L_x&=&{1\over 2}(L_+ + L_-)={\hbar\over\sqrt{2}}\left(\matrix...
...r\over\sqrt{2}i}\left(\matrix{0&1&0\cr -1&0&1\cr 0&-1&0}\right)
\end{eqnarray*}


What is the dimension of the matrices for $\ell =2$?
Dimension 5. Derive the matrix operators for $\ell =2$.
Just do it.



Jim Branson 2013-04-22