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Table 3

The modelling results for the different kinematic components within the extraction apertures.

Extraction kin FWHM ΔV Hβ [OIII]λ5007 [OI]λ6300 Hα [NII]λ6583 [SII]λ6716,6731
Aperture (AP) Comp km s-1 km s-1 erg s-1 cm-2
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)

IDS-POS1

a N1 158 ± 26 –64 ± 22 8.36E-16 13.53 0.56 4.17 5.71 2.11
N2 482 ± 31 –41 ± 22 5.01E-15 6.41 0.36 2.99 2.74 1.52
B 1458 ± 157 –204 ± 79 0.33 1.92 0.24 2.295E-15 3.01 1.18

b N 212 ± 30 –12 ± 25 2.99E-16 11.68 1.06 7.73 7.32 4.34
I1 644 ± 28 –173 ± 32 1.20E-15 9.00 0.76 7.02 6.54 3.74
I2 623 ± 64 411 ± 46 2.08E-16 4.36 1.40 5.02 15.07 2.67

c N 431 ± 33 –16 ± 21 2.12E-15 3.52 0.79 3.93 2.77 2.64
B 1407 ± 59 111 ± 33 5.66E-16 5.34 1.94 6.44 19.32 5.72

d N1 193 ± 46 285 ± 25 2.87E-16 2.11 ... 5.35 4.31 1.64
N2 362 ± 53 95 ± 43 6.84E-16 7.35 0.15 3.15 1.41 0.89
I 876 ± 122 73 ± 48 3.70E-16 8.20 1.69 4.09 8.48 6.34

e N 63 ± 21 67 ± 24 3.43E-16 7.27 ... 1.67 0.65 ...

f N 38 ± 15 114 ± 27 ... 9.94E-16 ... ... ...

IDS-POS2

g N1 163 ± 22 –13 ± 23 9.46E-16 9.47 0.89 5.24 6.23 2.93
N2 392 ± 43 –166 ± 30 1.78E-15 5.75 0.31 4.80 3.25 2.26
I 856 ± 63 –73 ± 34 9.53E-16 12.57 1.27 8.36 16.75 7.87

h N 149 ± 23 –22 ± 23 1.26E-15 0.56 0.26 6.44 1.98 1.60
I 500 ± 26 94 ± 23 5.35E-15 2.70 0.87 6.96 8.00 4.48
B 1518 ± 116 –468 ± 10 0.33 0.54 0.2 8.57E-15 1.85 0.67

i N 111 ± 25 –77 ± 24 2.23E-16 8.97 ... 3.33 2.26 ...

j N 84 ± 32 –26 ± 23 3.18E-16 12.14 ... 4.10 2.05 ...

k N 95 ± 29 43 ± 27 ... 1.106E-15 ... ... ... ...

Notes. Column (1): aperture label as indicated in Fig. 3. Column (2): The label of the different components as defined in Sect. 3.2.1: N (narrow), I (intermediate), and B (broad). For those apertures with two components within the same FWHM range, these are indicated with numbers (e.g. N1 and N2 corresponding to the two narrow components detected in Ap-a). Columns (3) and (4): instrumentally-corrected line widths (FWHM) and shifts (ΔV) measure relative to galaxy rest frame (defined as z = 0.0373, RV13). The uncertainties in these values were estimated accounting for the uncertainties from the modelling and the systematic calibration errors (i.e. the uncertainty in the instrumental width and the wavelength calibration error). Column (3): Hβ flux in erg s-1 cm-2. From Cols. (4)–(10): ratios of the fluxes of the main emission lines to the Hβ line. The uncertainties in these ratios are typically 15 per cent, as estimated accounting for the 5 percent flux calibration uncertainty, and the uncertainties in the model fits themselves. However, there are some particular cases, mainly those kinematic components that make a small contribution to the flux, for which the uncertainty can be as high as 50 percent (for example, the B component of the AP-a). These line ratios are not corrected for reddening.

(⋆)

For these two apertures the contribution of the broad component (B) to the overall Hβ flux is negligible. Therefore, when such component is included in the modelling its properties are entirely unconstrained, leading to unrealistic line ratio values. For the broad component in these two apertures, the fluxes are given relative to the Hα line. In addition, when calculating the line ratios used later for the diagnostic line ratio diagrams we took the conservative approach of assuming an Hα to Hβ ratio of 3. Note that, since reddening effects are expected to be important at the locations in the galaxy covered by these extraction apertures (i.e. the Hβ flux will be in reality less than 3 times the Hα flux), the [OIII]/Hβ line ratios calculated are lower limits of the real values.

(†)

For these two extraction apertures, only the [OIII]λλ4959,5007 emission lines are detected. The table show the [OIII]λ5007 flux in units of erg s-1 cm-2.

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