Spectroscopic Mueller Metrix Polarimetry Based on Spectral Modulation and Division of Amplitude Demodulation

$D_{z n} (σ) / 16$	Detail expressions
$D_{0 n} (σ)$	$2 (2 m_{00} + m_{02} + m_{10}) + m_{12} + (2 m_{10} + m_{12}) c o s 4 α_{n} - 2 (2 m_{30} + m_{32}) s i n 2 α_{n} + (2 m_{20} + m_{22}) s i n 4 α_{n}$
$D_{1 n} (σ)$	$2 m_{01} + m_{11} (1 + c o s 4 α_{n}) - 2 m_{31} s i n 2 α_{n} + m_{21} s i n 4 α_{n}$
$D_{- 1 n} (σ)$	$2 m_{01} + m_{11} (1 + c o s 4 α_{n}) - 2 m_{31} s i n 2 α_{n} + m_{21} s i n 4 α_{n}$
$D_{2 n} (σ)$	$- m_{02} - m_{12} c o s^{2} 2 α_{n} + m_{32} s i n 2 α_{n} - m_{22} c o s 2 α_{n} s i n 2 α_{n} + i (m_{03} + m_{13} c o s^{2} 2 α_{n} - m_{33} s i n 2 α_{n} + m_{23} c o s 2 α_{n} s i n 2 α_{n})$
$D_{- 2 n}$ $(σ)$	$- m_{02} - m_{12} c o s^{2} 2 α_{n} + m_{32} s i n 2 α_{n} - m_{22} c o s 2 α_{n} s i n 2 α_{n} - i (m_{03} + m_{13} c o s^{2} 2 α_{n} - m_{33} s i n 2 α_{n} + m_{23} c o s 2 α_{n} s i n 2 α_{n})$

Table 2. The detail expressions of the $D_{z n}^{r e f}$ coefficients

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Table 2. The detail expressions of the $D_{z n}^{r e f}$ coefficients

$D_{z n} (σ) / 16$	Detail expressions
$D_{0 n} (σ)$	$2 (2 + \sqrt[]{2}) + 1 / 2 + (\sqrt[]{2} + 1 / 2) c o s 4 α_{n} + (\sqrt[]{2} + 1 / 2) s i n 4 α_{n}$
$D_{1 n} (σ)$	$\sqrt[]{2} + 1 / 2 (1 + c o s 4 α_{n}) + 1 / 2 s i n 4 α_{n}$
$D_{- 1 n} (σ)$	$\sqrt[]{2} + 1 / 2 (1 + c o s 4 α_{n}) + 1 / 2 s i n 4 α_{n}$
$D_{2 n} (σ)$	$- \sqrt[]{2} / 2 - 1 / 2 c o s^{2} 2 α_{n} - 1 / 2 c o s 2 α_{n} s i n 2 α_{n}$
$D_{- 2 n}$ $(σ)$	$- \sqrt[]{2} / 2 - 1 / 2 c o s^{2} 2 α_{n} - 1 / 2 c o s 2 α_{n} s i n 2 α_{n}$

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Zhongxun DENG, Naicheng QUAN, Siyuan LI, Chunmin ZHANG. Spectroscopic Mueller Metrix Polarimetry Based on Spectral Modulation and Division of Amplitude Demodulation[J]. Acta Photonica Sinica, 2024, 53(4): 0430004

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