Table 4
Comparing the parameters of selected emission and absorption components.
| Comp. | NH | nHr2 | vmic | vout | E.M. | r | |||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| (1025 m−2) | (1044 m−1) | (km s−1) | (km s−1) | (1070 m−3) | (pc) | ||||||||
| EM 1 | 9.7 ± 1.3 | 5.7 ± 0.3 | 400 ± 30 | −47 ± 4 | 1.8 ± 0.6 | 1–3‡ | |||||||
| B | 0.69 ± 0.09 | 5.2 ± 0.8 | 49 ± 14 | −550 ± 40 | – | <0.23 or 13–20† | |||||||
| UV 1 |  |
 |
– | −1160 | – |  |
|||||||
| EM 2 | 30 ± 7 | 87 ± 11 | <280 | −420 ± 30 | 16 ± 10 | 1–3‡ | |||||||
| A | 0.26 ± 0.08 | 36 ± 12 | 150 ± 30 | −570 ± 40 | – | 31–50† | |||||||
Notes. Results from this work and (‡) Peterson et al. (2013) are used for the narrow emission components (EM 1 and 2 in Model T). The warm absorber components (A and B) are from Mao et al. (2017) and (†) Ebrero et al. (2016). The UV absorption component 1 is from Arav et al. (2015). We do not compare the ionization parameter, because it can vary due to the change in the ionizing luminosity. The emission measure (E.M.) is calculated via ne nH 4πCcovr2 NH∕nH.
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