Table A.1.
Photoionisation model predictions
Aperture | E(B-V) | [OIII]λ4363 | [OIII]λ5007 | [NII]λ5755 | [NII]λ6584 | [SII]λ6725 | [SII]![]() |
12+log(O/H) | log(N/O) | T[OIII] | T[NII] | ne |
---|---|---|---|---|---|---|---|---|---|---|---|---|
K | K | cm−3 | ||||||||||
1 | 0.074±0.012 | 0.144±0.014 | 6.000±0.215 | 0.019±0.001 | 1.437±0.114 | 1.598±0.047 | 1.316±0.056 | 8.68±0.15 | -0.86±0.11 | 16565±875 | 9508±312 | 149±79 |
2 | 0.155±0.015 | 0.141±0.012 | 5.802±0.588 | 0.017±0.001 | 1.396±0.044 | 1.507±0.051 | 1.396±0.026 | 8.61±0.13 | -0.85±0.11 | 16739±1196 | 9236±225 | 34±36 |
3 | 0.054±0.013 | 0.135±0.015 | 6.043±0.251 | 0.020±0.002 | 1.044±0.042 | 1.467±0.060 | 1.349±0.048 | 8.76±0.11 | -1.03±0.09 | 16058±1071 | 11185±448 | 100±63 |
4 | 0.034±0.013 | 0.158±0.012 | 7.290±0.251 | 0.018±0.002 | 1.012±0.048 | 1.359±0.071 | 1.382±0.027 | 8.69±0.10 | -1.00±0.08 | 15801±699 | 10822±543 | 51±34 |
5 | 0.063±0.018 | 0.142±0.008 | 7.199±0.322 | 0.016±0.002 | 0.991±0.062 | 1.196±0.056 | 1.343±0.033 | 8.77±0.12 | -0.99±0.08 | 15064±493 | 10325±565 | 109±41 |
6 | 0.046±0.017 | 0.143±0.010 | 6.885±0.319 | 0.019±0.001 | 1.086±0.063 | 1.326±0.078 | 1.321±0.036 | 8.69±0.12 | -0.98±0.11 | 15433±641 | 10656±344 | 141±52 |
7 | 0.101±0.014 | 0.162±0.009 | 7.342±0.323 | 0.019±0.001 | 1.070±0.067 | 1.419±0.059 | 1.341±0.036 | 8.68±0.09 | -1.00±0.08 | 15938±501 | 10743±353 | 114±50 |
8 | 0.087±0.021 | 0.128±0.014 | 5.665±0.326 | 0.020±0.001 | 1.291±0.112 | 1.589±0.088 | 1.369±0.046 | 8.76±0.15 | -0.93±0.11 | 16181±1037 | 10134±391 | 74±60 |
9 | 0.031±0.013 | 0.145±0.006 | 6.900±0.316 | 0.020±0.002 | 1.195±0.069 | 1.423±0.072 | 1.394±0.021 | 8.72±0.10 | -0.94±0.10 | 15453±442 | 10495±516 | 40±33 |
10 | 0.105±0.016 | 0.115±0.019 | 4.557±0.208 | 0.020±0.002 | 1.169±0.079 | 1.632±0.074 | 1.411±0.016 | 8.56±0.20 | -0.98±0.11 | 16888±1484 | 10580±530 | ≲35 |
Nucleus | 0.186±0.033 | 0.086±0.014 | 6.550±0.310 | 0.021±0.003 | 1.497±0.157 | 0.920±0.059 | 1.242±0.138 | 8.66±0.11 | -0.56±0.08 | 12772±785 | 9825±658 | 301±270 |
11 | 0.000±0.046 | 0.146±0.021 | 5.941±0.387 | N/A | 1.271±0.183 | 1.455±0.082 | 1.335±0.017 | 8.53±0.17 | -0.85±0.15 | 16899±1339 | N/A | 115±22 |
12 | 0.132±0.015 | 0.113±0.014 | 3.570±0.170 | N/A | 1.350±0.061 | 1.865±0.085 | 1.450±0.050 | 8.52±0.14 | -0.87±0.11 | 19540±1235 | N/A | 16±34 |
13 | 0.000±0.038 | 0.083±0.023 | 3.197±0.325 | N/A | 1.378±0.166 | 1.973±0.228 | 1.417±0.054 | 8.71±0.24 | -0.89±0.14 | 17766±2661 | N/A | 34±47 |
14 | 0.031±0.025 | 0.175±0.035 | 6.901±0.531 | N/A | 1.244±0.104 | 1.684±0.126 | 1.330±0.029 | 8.53±0.15 | -0.94±0.11 | 17197±2124 | N/A | 129±42 |
15 | 0.077±0.041 | 0.198±0.024 | 7.222±0.808 | N/A | 0.914±0.115 | 1.480±0.183 | 1.316±0.025 | 8.40±0.12 | -0.94±0.13 | 17989±1652 | N/A | 145±34 |
16 | 0.023±0.015 | 0.271±0.040 | 8.844±0.387 | N/A | 0.647±0.072 | 1.382±0.319 | N/A | 8.37±0.08 | -1.00±0.11 | 18829±1648 | N/A | N/A |
17 | 0.029±0.020 | 0.222±0.017 | 8.941±0.404 | N/A | 1.123±0.102 | 1.339±0.146 | 1.429±0.061 | 8.49±0.05 | -0.87±0.12 | 16910±754 | N/A | 33±48 |
18 | 0.121±0.012 | 0.102±0.023 | 3.917±0.210 | N/A | 1.097±0.058 | 1.602±0.191 | 1.466±0.030 | 8.56±0.24 | -0.93±0.13 | 17299±2055 | N/A | ≲75 |
19 | 0.027±0.044 | 0.090±0.028 | 2.626±0.481 | N/A | 1.245±0.283 | 1.125±0.378 | 1.386±0.039 | 8.39±0.30 | -0.86±0.28 | 18925±3439 | N/A | 48±45 |
20 | 0.077±0.031 | 0.087±0.016 | 3.075±0.420 | N/A | 1.494±0.282 | 1.888±0.284 | 1.396±0.039 | 8.60±0.25 | -0.84±0.20 | 18398±2835 | N/A | 41±45 |
21 | 0.126±0.059 | 0.201±0.033 | 8.234±1.289 | N/A | 0.716±0.126 | 0.947±0.164 | 1.372±0.028 | 8.44±0.13 | -0.94±0.16 | 16972±1929 | N/A | 70±38 |
22 | 0.000±0.007 | 0.154±0.012 | 7.099±0.143 | N/A | 0.776±0.038 | 1.164±0.338 | N/A | 8.44±0.18 | -0.97±0.17 | 15798±608 | N/A | N/A |
Notes. Model predictions of the O/H and N/O relative abundances, the electron temperatures, T[OIII] and T[NII] and electron densities ne inferred from the [SII] ratio. The observed, extinction corrected line fluxes used in the models are quoted relative to Hβ. E(B-V) values were inferred from Hα/Hβ. The spatial location of the apertures can be seen in Fig. 3. Apertures 3 to 9 cover the edge of the ionised bubble. The top (lower) part of the table comprises the apertures in which [NII]λ5755 is detected (undetected). N/A in the [SII]
column means that the doublet ratio could not be measured accurately due to residual sky artefacts. The solar abundances are 12+log(O/H) = 8.69±0.04 and log(N/O) = -0.86±0.07 for the Sun (Asplund et al. 2021).
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