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Table E.1

Results for the RingI60 models with r0 = 100.8 mas using different zp-corrections.

Σzp Σint ΣiX/ΣQϕ${{\rm{\Sigma }}_{i'}}X/{\rm{\Sigma }}Q_\phi ^\prime $ ΣiQxxx/ΣQϕ[%]${{\rm{\Sigma }}_{i'}}{Q_{xxx}}/{\rm{\Sigma }}Q_\phi ^\prime [{\rm{\% }}]$
Σi Σi${{\rm{\Sigma }}_{i'}}$ Qϕ Q P Q000 Q090 Q180
intrinsic parameters
Σ 100. +42.1 100. −0.7 +28.1 −13.4
PSFAO convolved parameters
Σ 55.9 +41.4 70.2 +3.2 +20.5 −2.8
Σ1 0.2 −0.2 0.3 0.0 0.0 −0.2
Σ2 55.2 +29.3 57.5 +0.3 +17.3 −5.6
Σ3 0.5 +12.2 12.4 +3.0 +3.2 +3.0
Σzp: whole system
Σ Σ 55.8 0.0 82.6 −6.6 +9.6 −13.6
Σ Σ1 0.2 −18.4 18.4 −4.2 −4.9 −5.1
Σ Σ2 55.2 +18.1 61.7 −2.3 +14.4 −8.6
Σ Σ3 0.5 +0.3 2.4 0.0 +0.2 0.0
Σzp : central star
Σ1 Σ 55.8 +41.8 70.4 +3.4 +20.6 −2.6
Σ1 Σ1 0.2 0.0 0.4 0.0 0.0 −0.1
Σ1 Σ2 55.2 +29.7 57.5 +0.3 +17.3 −5.5
Σ1 Σ3 0.5 +12.4 12.5 +3.0 +3.2 +3.0
Σzp: disk
Σ2 Σ 55.8 −66.3 140. −22.3 −7.7 −31.1
Σ2 Σ1 0.2 −47.6 47.6 −11.0 −12.7 −12.9
Σ2 Σ2 55.1 0.0 73.2 −6.6 +9.6 −13.4
Σ2 Σ3 0.5 −18.7 18.9 −4.8 −4.6 −4.8
Σzp: disk and halo
Σ2+3 Σ 55.8 −32.9 109. −14.4 +1.1 −22.3
Σ2+3 Σ1 0.2 −32.8 32.9 −7.6 −8.8 −8.9
Σ2+3 Σ2 55.1 +9.1 67.1 −4.4 +12.0 −10.9
Σ2+3 Σ3 0.5 −9.1 9.5 −2.4 −2.2 −2.4
Σzp : halo
Σ3 Σ 55.8 −1.2 83.3 −6.8 +9.3 −13.9
Σ3 Σ1 0.2 −18.9 18.9 −4.3 −5.0 −5.2
Σ3 Σ2 55.2 +17.7 61.9 −2.4 +14.3 −8.6
Σ3 Σ3 0.5 0.0 2.5 −0.1 +0.1 −0.1

Notes. The table lists integrated polarization X = Qϕ, Q, P and quadrant polarization values Qxxx for different integration regions Σint of the PSFAO convolved model, and for corresponding zp-corrected models using different zp-correction regions Σzp. The parameters ΣiX${{\rm{\Sigma }}_{i'}}X$ and ΣiXxxx${{\rm{\Sigma }}_{i'}}{X_{xxx}}$ for the table columns stand for intrinsic values X = X′ and Qxxx=Qxxx${Q_{xxx}} = {{Q'}_{xxx}}$, for convolved values X and Qxxx, and for values Xzi and Qxxxzi$Q_{xxx}^{zi}$ with zp-corrections based on region Σzp = Σi, integrated in region Σzp=Σi${{\rm{\Sigma }}_{zp}} = {{\rm{\Sigma }}_i}$ (Table A.2). All values are normalized to the intrinsic azimuthal polarization ΣQϕ${\rm{\Sigma }}Q_\phi ^\prime $.

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