Open Access
Table A.1
Dictionary of all defined quantities, with complex quantities in bold.
| Notation | Meaning | Reference |
|---|---|---|
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complex polarized intensity in channel i | Eq. (1), Sect. 2.2 |
| ψi | polarization angle in channel i | Sect. 2.2 |
| ν0 | reference frequency | Sect. 2.2 |
| P0 | polarized intensity map at the reference frequency | Sect. 2.5 |
| I0 | total intensity map at the reference frequency | Sect. 3.2 |
| p0 | polarization fraction p0 = P0/I0 at the reference frequency | Sect. 3.2 |
| T, β, εν | temperature, spectral index and emissivity of aligned grains | Eq. (3) |
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pivot temperature and spectral index defining the pivot SED | Eq. (6), Sect. 2.2 |
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value of the pivot SED in channel i of frequency νi | Eq. (6) |
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order n of spectral gradients, for s ∈ {T, β} and for T and β | Eq. (7) |
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polarization-weighted complex spin-moments of order n | Eq. (8) |
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intensity-weighted moments of order n | Eq. (11) |
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difference between moments characterizing depolarization effects | Eq. (12) |
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mean values over the sky weighted by ![]() |
Eq. (17), Sects. 2.4, 2.5 |
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correction to the polarization efficiency in channel i | Sects. 4.1 & 4.3 |
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mean complex SED normalized to the reference frequency | Eq. (16) and (42), Sects. 2.4 & 4.3 |
| Ri | complex residual map for channel i | Eq. (18) |
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residual map of polarized intensity in channel i | Eq. (21) |
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residual map of polarization angle in channel i | Eq. (22) |
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residual map of dust emissivity in polarization | Eq. (23) |
| Cov(X, Y) | covariance of X and Y maps, weighted by ![]() |
Eq. (25), Sect. 2.6 |
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covariance of and ![]() |
Eq. (26) |
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covariance of and ![]() |
Eq. (27) |
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mixed covariance of and ![]() |
Eq. (28) |
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covariance of and , and its estimate |
Eqs.(29) and (39) |
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complex covariance of Ri and Rj | Eq. (30) |
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Pearson correlation coefficients between residual maps (i ≠ j) | Table 1, Sect. 4.4 |
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standard deviations fitting the spectral dependence of ![]() |
Sect. 5.1 |
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standard deviations fitting the spectral dependence of ![]() |
Sect. 5.1 |
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mixed covariance fitting the spectral dependence of ![]() |
Sect 6.1 |
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parameters characteristic of the magnetic field model | Appendix C |
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![$\[\mathbf{P}_{i}=Q_{i}+\dot{\mathbb{i}} U_{i}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq216.png)
![$\[\overline{T}, \overline{\beta}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq217.png)
![$\[\overline{\varepsilon}_{i}=\overline{\varepsilon}_{\nu_{i}}(\overline{\beta}, \overline{T})\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq218.png)
![$\[a_{i, n}^{s}, a_{i, n}^{T}, a_{i, n}^{\beta}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq219.png)
![$\[\boldsymbol{\mathcal{W}}_{n}^{s}, \boldsymbol{\mathcal{W}}_{n}^{\beta}, \boldsymbol{\mathcal{W}}_{n}^{T}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq220.png)
![$\[\omega_{n}^{s}, \omega_{n}^{\beta}, \omega_{n}^{T}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq221.png)
![$\[\boldsymbol{\Delta}_{n}^{s}=\boldsymbol{\mathcal{W}}_{n}^{s}-\omega_{n}^{s}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq222.png)
![$\[\overline{\boldsymbol{\mathcal{W}}}_{n}^{s}, \overline{\omega}_{n}^{s}, \overline{\boldsymbol{\Delta}}_{n}^{s}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq223.png)
![$\[P_{0}^{2}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq224.png)
![$\[\tilde{\rho}_{i}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq225.png)
![$\[\overline{\mathbf{r}}_{i}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq226.png)
![$\[R_{i}^{P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq227.png)
![$\[R_{i}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq228.png)
![$\[R_{i}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq229.png)
![$\[P_{0}^{2}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq230.png)
![$\[c_{i j}^{P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq231.png)
![$\[R_{i}^{P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq232.png)
![$\[R_{j}^{P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq233.png)
![$\[c_{i j}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq234.png)
![$\[R_{i}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq235.png)
![$\[R_{j}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq236.png)
![$\[c_{i j}^{\psi P}, c_{i j}^{P \psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq237.png)
![$\[R_{i}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq238.png)
![$\[R_{j}^{P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq239.png)
![$\[c_{i j}^{\varepsilon}, \hat{c}_{i j}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq240.png)
![$\[R_{i}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq241.png)
![$\[R_{j}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq242.png)
![$\[\mathbf{c}_{i j}^{\mathbf{P}}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq243.png)
![$\[\rho_{i j}^{\mathbf{P}}, \rho_{i j}^{P}, \rho_{i j}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq244.png)
![$\[\sigma_{s}^{\psi}, \sigma_{T}^{\psi}, \sigma_{\beta}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq245.png)
![$\[c_{i j}^{\psi}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq246.png)
![$\[\sigma_{s}^{\varepsilon}, \sigma_{T}^{\varepsilon}, \sigma_{\beta}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq247.png)
![$\[c_{i j}^{\varepsilon}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq248.png)
![$\[\Sigma_{T}^{\psi P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq249.png)
![$\[c_{i j}^{\psi P}\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq250.png)
![$\[\overline{\eta}, \eta(p)\]$](/articles/aa/full_html/2026/01/aa56491-25/aa56491-25-eq251.png)