This shows you the differences between two versions of the page.
| Next revision | Previous revision | ||
| topic:optics:characterization:retardance [2020/09/03 16:14] – created samuel | topic:optics:characterization:retardance [2020/09/03 16:31] (current) – [Mueller Matrix method] Some index errors. samuel | ||
|---|---|---|---|
| Line 12: | Line 12: | ||
| ==== Mueller Matrix method ==== | ==== Mueller Matrix method ==== | ||
| + | This is based on \cite{Hui.OSullivan: | ||
| $$ \begin{bmatrix} s_1 \\ s_2 \\ s_3 \end{bmatrix} | $$ \begin{bmatrix} s_1 \\ s_2 \\ s_3 \end{bmatrix} | ||
| + | |||
| + | If $\mathbf{s}_i$ is the basis vectors with a 1 on position $i$, all three output stokes vectors, will form the Mueller matrix. | ||
| + | |||
| + | Also two independent input polarization states (no need to be orthogonal) allow determining the Mueller matrix as follows. | ||
| + | Measure $\mathbf{s}_a$ and $\mathbf{s}_b$ for two independent input polarizations. $\mathbf{s_1} = \mathbf{s_a}$ and then we can find a orthogonal vector to $\mathbf{s_1}$ and $\mathbf{s_b}$ through the cross-product. $$ \mathbf{s_3} = \mathbf{s_1} \times \mathbf{s_b} $$ | ||
| + | The third vector can then be found by using the orthogonality through $$\mathbf{s_2} = \mathbf{s_3} \times \mathbf{s_1} $$. | ||
| + | |||
| + | |||