琼斯运算

${\displaystyle {\begin{pmatrix}1&0\\0&0\end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}0&0\\0&1\end{pmatrix}}}$ 

${\displaystyle {\frac {1}{2}}{\begin{pmatrix}1&1\\1&1\end{pmatrix}}}$ 

${\displaystyle {\frac {1}{2}}{\begin{pmatrix}1&-1\\-1&1\end{pmatrix}}}$ 

${\displaystyle {\frac {1}{2}}{\begin{pmatrix}1&i\\-i&1\end{pmatrix}}}$ 

${\displaystyle {\frac {1}{2}}{\begin{pmatrix}1&-i\\i&1\end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}\cos ^{2}\Psi &\cos \Psi \sin \Psi \\\sin \Psi \cos \Psi &\sin ^{2}\Psi \end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}e^{-i\Gamma /2}&0\\0&e^{i\Gamma /2}\end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}e^{i\Gamma /2}&0\\0&e^{-i\Gamma /2}\end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}\cos(\Gamma /2)&i\sin(\Gamma /2)\\i\sin(\Gamma /2)&\cos(\Gamma /2)\end{pmatrix}}}$ 

${\displaystyle {\begin{pmatrix}e^{-i\Gamma /2}\cos ^{2}\Psi +e^{i\Gamma /2}\sin ^{2}\Psi &-i\sin(\Gamma /2)\sin(2\Psi )\\-i\sin(\Gamma /2)\sin(2\Psi )&e^{-i\Gamma /2}\sin ^{2}\Psi +e^{i\Gamma /2}\cos ^{2}\Psi \end{pmatrix}}}$