Table 2.

Emission-line properties derived from the line fitting of the GNIRS spectrum.

LineFluxLine centroidFWHM
(10−19 erg s−1 cm−2)(rest frame, Å)(km s−1)
H β278 ± 584862.4 ± 0.4264 ± 63
|$\rm {[O\,{\small III}]} \lambda 4959$| (narrow)936 ± 1254958.7 ± 0.2394 ± 40
|$\rm {[O\,{\small III}]}$| λ4959 (broad)501 ± 1574949 ± 21170 ± 389
|$\rm {[O\,{\small III}]}$| λ5007 (narrow)2084 ± 2495006.8 ± 0.2354 ± 31
|$\rm {[O\,{\small III}]}$| λ5007 (broad)1099 ± 2624998 ± 21376 ± 356
|$\rm {[N\,{\small II}]}$| λ6548847 ± 1076547.4 ± 0.5756 ± 78
H α2312 ± 1086562.6 ± 0.3604 ± 30
|$\rm {[N\,{\small II}]}$| λ65842120 ± 1496583.7 ± 0.5756 ± 78
|$\rm {[S\,{\small II}]}$| λ6716 (a)307 ± 586715.9 ± 0.6319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731327 ± 736731.4 ± 0.6413 ± 92
|$\rm {[S\,{\small II}]}$| λ6716 (b)307 ± 586716.0 ± 0.5319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731282 ± 596731.5 ± 0.5319 ± 79
LineFluxLine centroidFWHM
(10−19 erg s−1 cm−2)(rest frame, Å)(km s−1)
H β278 ± 584862.4 ± 0.4264 ± 63
|$\rm {[O\,{\small III}]} \lambda 4959$| (narrow)936 ± 1254958.7 ± 0.2394 ± 40
|$\rm {[O\,{\small III}]}$| λ4959 (broad)501 ± 1574949 ± 21170 ± 389
|$\rm {[O\,{\small III}]}$| λ5007 (narrow)2084 ± 2495006.8 ± 0.2354 ± 31
|$\rm {[O\,{\small III}]}$| λ5007 (broad)1099 ± 2624998 ± 21376 ± 356
|$\rm {[N\,{\small II}]}$| λ6548847 ± 1076547.4 ± 0.5756 ± 78
H α2312 ± 1086562.6 ± 0.3604 ± 30
|$\rm {[N\,{\small II}]}$| λ65842120 ± 1496583.7 ± 0.5756 ± 78
|$\rm {[S\,{\small II}]}$| λ6716 (a)307 ± 586715.9 ± 0.6319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731327 ± 736731.4 ± 0.6413 ± 92
|$\rm {[S\,{\small II}]}$| λ6716 (b)307 ± 586716.0 ± 0.5319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731282 ± 596731.5 ± 0.5319 ± 79

Note. Letter (a) refers to the line fit of the [S ii] λλ6716, 6731 doublet in which only the centroids ratio was fixed to the theoretical value while letter (b) indicates the fit in which the FWHM of [S ii] λ6731 was matched to the FWHM of [S ii] λ6716 calculated in fit (a).

Table 2.

Emission-line properties derived from the line fitting of the GNIRS spectrum.

LineFluxLine centroidFWHM
(10−19 erg s−1 cm−2)(rest frame, Å)(km s−1)
H β278 ± 584862.4 ± 0.4264 ± 63
|$\rm {[O\,{\small III}]} \lambda 4959$| (narrow)936 ± 1254958.7 ± 0.2394 ± 40
|$\rm {[O\,{\small III}]}$| λ4959 (broad)501 ± 1574949 ± 21170 ± 389
|$\rm {[O\,{\small III}]}$| λ5007 (narrow)2084 ± 2495006.8 ± 0.2354 ± 31
|$\rm {[O\,{\small III}]}$| λ5007 (broad)1099 ± 2624998 ± 21376 ± 356
|$\rm {[N\,{\small II}]}$| λ6548847 ± 1076547.4 ± 0.5756 ± 78
H α2312 ± 1086562.6 ± 0.3604 ± 30
|$\rm {[N\,{\small II}]}$| λ65842120 ± 1496583.7 ± 0.5756 ± 78
|$\rm {[S\,{\small II}]}$| λ6716 (a)307 ± 586715.9 ± 0.6319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731327 ± 736731.4 ± 0.6413 ± 92
|$\rm {[S\,{\small II}]}$| λ6716 (b)307 ± 586716.0 ± 0.5319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731282 ± 596731.5 ± 0.5319 ± 79
LineFluxLine centroidFWHM
(10−19 erg s−1 cm−2)(rest frame, Å)(km s−1)
H β278 ± 584862.4 ± 0.4264 ± 63
|$\rm {[O\,{\small III}]} \lambda 4959$| (narrow)936 ± 1254958.7 ± 0.2394 ± 40
|$\rm {[O\,{\small III}]}$| λ4959 (broad)501 ± 1574949 ± 21170 ± 389
|$\rm {[O\,{\small III}]}$| λ5007 (narrow)2084 ± 2495006.8 ± 0.2354 ± 31
|$\rm {[O\,{\small III}]}$| λ5007 (broad)1099 ± 2624998 ± 21376 ± 356
|$\rm {[N\,{\small II}]}$| λ6548847 ± 1076547.4 ± 0.5756 ± 78
H α2312 ± 1086562.6 ± 0.3604 ± 30
|$\rm {[N\,{\small II}]}$| λ65842120 ± 1496583.7 ± 0.5756 ± 78
|$\rm {[S\,{\small II}]}$| λ6716 (a)307 ± 586715.9 ± 0.6319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731327 ± 736731.4 ± 0.6413 ± 92
|$\rm {[S\,{\small II}]}$| λ6716 (b)307 ± 586716.0 ± 0.5319 ± 79
|$\rm {[S\,{\small II}]}$| λ6731282 ± 596731.5 ± 0.5319 ± 79

Note. Letter (a) refers to the line fit of the [S ii] λλ6716, 6731 doublet in which only the centroids ratio was fixed to the theoretical value while letter (b) indicates the fit in which the FWHM of [S ii] λ6731 was matched to the FWHM of [S ii] λ6716 calculated in fit (a).

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