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Table 3.

Hα-based SFRs and metallicity estimated from the IFU emission lines.

Demarcation line approach
BPT rainbow method
Object fHα(a) SFRHα(b) Class (c) fHα(a) SFRHα(b) 12 + log(O/H) (d) αO/H(e)
[10−16 erg s−1 cm−2] [M yr−1] [10−16 erg s−1 cm−2] [M yr−1] [] []
HE 0021−1819 359 ± 36 1.3 ± 0.1 MS 342 ± 34 1.2 ± 0.1 8.89 ± 0.02 −0.031 ± 0.010
HE 0040−1105 16 ± 2 0.03 ± 0.00 AGN < 41 < 0.1 8.85 ± 0.02 0.040 ± 0.016
HE 0045−2145 5672 ± 567 3.1 ± 0.3 LMS 4687 ± 477 2.5 ± 0.3 9.16 ± 0.02 −0.018 ± 0.003
HE 0108−4743 8594 ± 859 5.9 ± 0.6 MS 8251 ± 825 5.7 ± 0.6 9.05 ± 0.01 −0.055 ± 0.009
HE 0114−0015 978 ± 98 2.5 ± 0.3 LMS 901 ± 90 2.3 ± 0.2 9.06 ± 0.02 −0.007 ± 0.011
HE 0119−0118 1107 ± 111 4.1 ± 0.4 MS 1006 ± 101 3.8 ± 0.4 8.99 ± 0.01 0.026 ± 0.020
HE 0150−0344 3961 ± 396 10.5 ± 1.0 8.88 ± 0.02 −0.029 ± 0.005
HE 0203−0031 71 ± 7 0.16 ± 0.02 AGN+SF < 202 < 0.5 9.08 ± 0.02 −0.006 ± 0.003
HE 0212−0059 4163 ± 416 3.5 ± 0.4 MS 3978 ± 398 3.4 ± 0.3 8.99 ± 0.00 −0.050 ± 0.013
HE 0224−2834 368 ± 37 1.7 ± 0.2 MS+AGN 397 ± 40 1.8 ± 0.2 8.88 ± 0.01 −0.006 ± 0.007
HE 0227−0913 2970 ± 297 1.0 ± 0.1 MS 2933 ± 293 0.9 ± 0.1 8.96 ± 0.01 −0.017 ± 0.007
HE 0232−0900 8226 ± 823 19.0 ± 1.9 MS 8197 ± 820 19.0 ± 1.9 9.00 ± 0.01 −0.017 ± 0.004
HE 0253−1641 197 ± 20 0.24 ± 0.02 MS 232 ± 23 0.28 ± 0.03 8.97 ± 0.02 −0.025 ± 0.023
HE 0345+0056 3474 ± 348 4.1 ± 0.4 SF 3477 ± 348 4.1 ± 0.4 8.81 ± 0.09 0.066 ± 0.073
HE 0351+0240 143 ± 14 0.23 ± 0.02 AGN < 240 < 0.4 8.80 ± 0.03 −0.010 ± 0.013
HE 0412−0803 93 ± 9 0.17 ± 0.02 AGN < 192 < 0.3 8.85 ± 0.02 0.009 ± 0.007
HE 0429−0247 262 ± 26 0.6 ± 0.1 AGN < 338 < 0.7 8.80 ± 0.02 0.016 ± 0.015
HE 0433−1028 5997 ± 600 9.3 ± 0.9 MS+SF 6700 ± 671 10.4 ± 1.0 8.97 ± 0.01 −0.049 ± 0.009
HE 0853+0102 407 ± 41 1.4 ± 0.1 MS 381 ± 38 1.3 ± 0.1 8.89 ± 0.02 −0.005 ± 0.021
HE 0853−0126 142 ± 14 0.6 ± 0.1 SF 130 ± 13 0.6 ± 0.1 8.60 ± 0.16 0.130 ± 0.154
HE 0934+0119 650 ± 65 2.1 ± 0.2 MS+SF 599 ± 60 1.9 ± 0.2 8.92 ± 0.02 −0.098 ± 0.011
HE 0949−0122 26 ± 3 0.01 ± 0.00 AGN < 214 < nan 8.90 ± 0.04 0.049 ± 0.039
HE 1011−0403 328 ± 33 1.4 ± 0.1 LMS 294 ± 29 1.3 ± 0.1 9.03 ± 0.01 −0.022 ± 0.014
HE 1017−0305 353 ± 35 1.1 ± 0.1 LMS 340 ± 34 1.1 ± 0.1 9.00 ± 0.02 −0.007 ± 0.021
HE 1029−1831 4689 ± 469 9.4 ± 0.9 SF 3732 ± 377 7.5 ± 0.8 9.12 ± 0.01 −0.099 ± 0.006
HE 1107−0813 121 ± 12 0.5 ± 0.1 MS+AGN 115 ± 12 0.49 ± 0.05 9.08 ± 0.02 −0.003 ± 0.006
HE 1108−2813 6094 ± 609 4.2 ± 0.4 MS+SF 5840 ± 587 4.1 ± 0.4 9.01 ± 0.01 −0.110 ± 0.008
HE 1126−0407 195 ± 20 1.0 ± 0.1 MS 217 ± 22 1.1 ± 0.1 9.08 ± 0.03 −0.048 ± 0.022
HE 1237−0504 1501 ± 150 0.14 ± 0.01 LMS 3249 ± 425 0.31 ± 0.04 9.10 ± 0.00 −0.144 ± 0.025
HE 1248−1356 2766 ± 277 0.7 ± 0.1 MS 3034 ± 303 0.8 ± 0.1 9.05 ± 0.01 −0.128 ± 0.012
HE 1310−1051 1294 ± 129 1.9 ± 0.2 SF 1258 ± 127 1.8 ± 0.2 8.84 ± 0.07 0.010 ± 0.049
HE 1330−1013 763 ± 76 0.45 ± 0.05 MS 716 ± 72 0.42 ± 0.04 9.13 ± 0.04 −0.146 ± 0.053
HE 1338−1423 742 ± 74 1.6 ± 0.2 AGN 1319 ± 135 2.9 ± 0.3 9.04 ± 0.06 −0.019 ± 0.075
HE 1353−1917 609 ± 61 0.9 ± 0.1 MS+A+S 594 ± 59 0.9 ± 0.1 8.96 ± 0.02 −0.119 ± 0.013
HE 1417−0909 6 ± 1 0.01 ± 0.00 AGN < 23 < 0.1 8.73 ± 0.08 0.106 ± 0.066
HE 2128−0221 154 ± 15 0.5 ± 0.1 MS 140 ± 14 0.49 ± 0.05 8.93 ± 0.04 −0.047 ± 0.020
HE 2211−3903 2419 ± 242 4.7 ± 0.5 MS+SF 2534 ± 253 4.9 ± 0.5 9.08 ± 0.01 −0.145 ± 0.010
HE 2222−0026 43 ± 4 0.19 ± 0.02 SF 34 ± 3 0.15 ± 0.02 8.80 ± 0.05 0.088 ± 0.050
HE 2233+0124 355 ± 36 1.4 ± 0.1 MS+AGN 339 ± 34 1.4 ± 0.1 9.05 ± 0.02 −0.057 ± 0.018
HE 2302−0857 1339 ± 134 3.7 ± 0.4 MS 1618 ± 162 4.4 ± 0.4 8.92 ± 0.01 −0.074 ± 0.013

Notes.

(a)

Integrated extinction-corrected Hα flux decontaminated by AGN contribution either using a demarcation line cut or the rainbow method presented here. Given the high S/N of the data the error is dominated by the systematics in the absolute photometric zero-point which is assumed to be 10%.

(b)

Hα-based SFR determined from the asscoicated Hα luminosity following the calibration of Calzetti et al. (2007), see Eq. (2).

(c)

Classification of the BPT in a (LINER) mixing sequence (L)MS, AGN cloud, SF cloud and any combination of the four.

(d)

Central oxygen abdundance on the Tremonti et al. (2004) metallicity scale determined through the N2S2 index following Eq. (5). A linear fit to the radial distribution is used to determine the central abdunance as the spatial coverages varies through the sample.

(e)

Slope of the linear metallicity gradient normalized to the effective radius of the respective galaxy as reported in Husemann et al. (2022).

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