Open Access
Table A.1.
Same as Table 1 but for the Teacup and J1356S. In the case of J1356S, the tabulated flux for Brγ corresponds to 3σ upper limit, as the line is not detected there.
| Nuclear Spectrum | ||||||
|---|---|---|---|---|---|---|
| J1430 | J356S | |||||
| Line | FWHM | Vs | Line Flux × 1015 | FWHM | Vs | Line Flux × 1015 |
| (km s−1) | (km s−1) | (erg cm−2 s−1) | (km s−1) | (km s−1) | (erg cm−2 s−1) | |
| Paα | 421 ± 4 | 12 ± 8 | 7.63 ± 1.15 | 702 ± 23 | -52 ± 26 | 0.57 ± 0.10 |
| Paα (b) | 1245 ± 41 | -100 ± 20 | 5.82 ± 0.97 | - | - | - |
| Brδ | 395 ± 27 | -2 ± 14 | 0.39 ± 0.07 | 472 ± 239 | -10 ± 144 | 0.01 ± 0.01 |
| Brδ (b) | 1180 ± 155 | -200 ± 105 | 0.28 ± 0.11 | - | - | - |
| Brγ | 321 ± 26 | -11 ± 12 | 0.42 ± 0.09 | - | - | 0.04* |
| Brγ (b) | 949 ± 79 | -13 ± 29 | 0.69 ± 0.19 | - | - | - |
| He I | 376 ± 47 | -20 ± 23 | 0.35 ± 0.89 | 939 ± 371 | 200 ± 182 | 0.13 ± 0.06 |
| He II | 549 ± 43 | 20 ± 25 | 0.50 ± 0.09 | 767 ± 258 | -119 ± 196 | 0.04 ± 0.02 |
| [Si VI] | 511 ± 41 | 61 ± 18 | 0.75 ± 0.20 | 939 ± 663 | 50 ± 753 | 0.04 ± 0.05 |
| [Si VI] (b) | 1175 ± 405 | 0 ± 237 | 0.39 ± 0.38 | - | - | - |
| H21-0S(1) | 560 ± 9 | 18 ± 10 | 0.68 ± 0.10 | 619 ± 68 | 20 ± 41 | 0.09 ± 0.02 |
| H21-0S(2) | 518 ± 15 | -14 ± 12 | 0.25 ± 0.04 | 502 ± 82 | 29 ± 50 | 0.03 ± 0.01 |
| H21-0S(3) | 596 ± 32 | -32 ± 24 | 0.75 ± 0.14 | 793 ± 143 | 204 ± 176 | 0.1 ± 0.06 |
| H21-0S(4) | 564 ± 123 | -95 ± 74 | 0.20 ± 0.08 | 1175 ± 181 | -79 ± 98 | 0.05 ± 0.01 |
| H21-0S(5) | 484 ± 48 | -9 ± 30 | 0.32 ± 0.07 | 733 ± 100 | -82 ± 60 | 0.06 ± 0.02 |
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