Table A.2.
Fluxes of the different components of the system derived from the R100 data cube, in units of [×10−18 erg s−1 cm−2].
| region | [S II] λ6716 + λ6731 | [S III] λ9069 | [S III] λ9531 | |
|---|---|---|---|---|
| main | 55.3 ± 6.8 | 17.2 ± 3.3 | 43.1 ± 4.1 | |
| south | 27.9 ± 3.6 | 6.8 ± 1.8 | 19.9 ± 2.3 | |
| north | 23.0 ± 3.1 | 8.5 ± 1.2 | 21.0 ± 1.4 | |
| s1 | 4.0 ± 0.8 | 2.0 ± 0.6 | 3.8 ± 0.8 | |
| s2 | 8.2 ± 1.0 | 1.5 ± 0.4 | 4.7 ± 0.6 | |
| s3 | 6.5 ± 1.4 | 2.4 ± 0.7 | 7.6 ± 0.8 | |
| n1 | 3.0 ± 0.6 | 1.1 ± 0.3 | 2.7 ± 0.3 | |
| n2 | 3.8 ± 0.6 | 1.1 ± 0.3 | 2.6 ± 0.3 | |
| n3 | 6.7 ± 0.9 | 1.1 ± 0.2 | 4.4 ± 0.3 | |
| c | 2.6 ± 0.4 | 0.6 ± 0.2 | 1.4 ± 0.3 | |
Notes. Fluxes of the different components identified in Fig. 1. Fluxes have been corrected for obscuration using a Cardelli et al. (1989) attenuation law as is described in Sec. 5.2.1. We report the total flux of the [S II] λ6716 + [S II] λ6731 doublet, since the two lines are not resolved in the R100 data.
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