Table 2.
Measurements from the nuclear spectrum using a model with three Gaussian components.
| Emission line | F1/F2/F3 | v1/v2/v3 | σ1/σ2/σ3 |
|---|---|---|---|
| (10−18 erg s−1 cm−2) | (km s−1) | (km s−1) | |
| Hβ | 403/254/44 | −47/−3/137 | 487/178/60 |
| [O III]λ5007 | 1632/1495/200 | −317/−27/144 | 662/210/46 |
| [O I]λ6300 | 1131/504/93 | −34/27/151 | 443/157/49 |
| Hα | 1182/1273/316 | −281/7/142 | 339/172/55 |
| [N II] λ6583 | 2855/1558/325 | −202/31/156 | 446/161/50 |
| [S II] λ6716 | 973/301/392 | 4/−8/150 | 264/90/62 |
| [S II] λ6731 | 1012/256/292 | 4/−8/150 | 264/90/62 |
Notes. Fi denotes the flux of the component i, vi the velocity of the peak of that component and σi its velocity dispersion (corrected for instrumental resolution). The three components have been sorted in this table based on their velocity dispersions.
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