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Table A.2.

Line fluxes for the sources and regions in the FoV1

Sp OII-R100 OII-R2700 Hβ-R100 Hβ-R2700 OIII-R100 OIII-R2700 Hα-R100 Hα-R2700 NII-R100 NII-R2700
E 8.71±0.48 8.52±0.43 4.50±0.17 4.46±0.24 15.49±0.19 14.48±0.28 21.03±0.33 18.59±0.56 5.54±0.27 4.52±0.48
E1c 8.08±0.56 8.91±0.56 4.65±0.19 4.77±0.29 15.46±0.22 14.47±0.34 22.91±0.52 18.57±0.71 5.24±0.43 4.12±0.61
Eext 10.04±0.56 10.77±0.83 15.38±1.512 13.82±2.34 0.14±2.64
ES 1.95±0.18 1.51±0.17 0.70±0.08 0.70±0.08 2.00±0.09 1.98±0.09 3.88±0.11 3.09±0.25 0.98±0.09 1.25±0.23
EN 4.74±0.24 4.39±0.25 2.81±0.10 2.42±0.14 10.26±0.11 9.14±0.16 11.88±0.20 10.49±0.32 3.33±0.17 1.85±0.27
ENa 1.15±0.07 1.41±0.11 0.73±0.04 0.86±0.07 2.93±0.05 2.95±0.08 3.02±0.05 3.34±0.20 0.81±0.04 0.88±0.19
ENb 1.86±0.12 1.35±0.10 1.00±0.05 0.87±0.05 3.47±0.05 3.10±0.06 4.06±0.10 3.39±0.12 1.21±0.08 0.56±0.10
ENc 0.40±0.05 0.35±0.07 0.20±0.04 0.14±0.03 0.91±0.04 0.69±0.03 0.99±0.05 0.76±0.06 0.22±0.04 0.16±0.05
W 3 1.28±0.28 4.93±0.52 1.08±0.41
W1c 1.10±0.24 2.78±0.32 3.02±0.49 1.13±0.26 1.32±0.41
Wext 2.12±0.66 7.35±0.64 6.00±0.74 5.77±0.78 3.01±0.68
C1 1.41±0.12 1.14±0.13 0.54±0.09 0.31±0.08 1.55±0.10 1.52±0.09 1.74±0.12 1.39±0.24 0.38±0.10 < 0.876
C2 0.54±0.10 0.47±0.11 0.31±0.07 1.59±0.09 1.27±0.06 1.07±0.122 0.88±0.13 < 0.465
C3 0.55±0.17 0.26±0.07 0.32±0.06 0.77±0.08 0.64±0.07 1.49±0.19 1.19±0.18 0.54±0.15
L1 0.49±0.11 0.30±0.07 0.28±0.05 3.17±0.08 2.95±0.06 1.28±0.12 1.29±0.12 < 0.429
L2 0.64±0.06 0.40±0.04
L3 0.70±0.09 0.77±0.05 0.50±0.12 0.49±0.12
L4 (0.74±0.06)4 (0.31±0.05)4 0.76±0.09 0.59±0.13 0.29±0.08
L5 0.71±0.10 0.41±0.05 3.16±0.12 2.56±0.06 1.89±0.232 1.55±0.11 < 0.565
L6 0.61±0.08 0.59±0.06 0.51±0.08 0.52±0.10

Notes. 1From the integrated spectra in the apertures defined in Fig. A.1, in units of 10−18 erg/s/cm−2. For E and W galaxies we also include values in apertures of 1 arcsec in diameter as in Álvarez-Márquez et al. (2023). No aperture corrections, nor 10 percent correction for R100 fluxes are applied. 2 The fit for the Hα -[NII] complex gives no flux for the [NII]lines. 3 For W, R100 Hβ flux is contaminated by the lens galaxy. For the Hα flux the R100 spectrum is preferred because the large velocity range covered by the aperture induces a significant increase of noise in the high resolution spectrum. 4 Difference between R100 and R2700 fluxes are larger than × 2, and not considered. The upper limits correspond to 3-σ the noise level.

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