Open Access

Table B.2.

Results from the analysis of high-resolution spectroscopy of the sample.

Target S/NHα S/N[OIII] FWHMHα FWHM[OIII] fout, Hα fout, [OIII]
[km/s] [km/s]
2MASSJ00114318+1428010 107 11 92 ± 1.5 90 ± 11 0.2 ± 0.09 -
AGC244381 10 - 70 ± 14 - - -
IC159 36 7 50 ± 5 100 ± 20 - -
IC5292 59 - 60 ± 3 - - -
LEDA1278497 22 4 110 ± 6 100 ± 40 - -
LEDA1397680 82 - 91 ± 1.2 - - -
LEDA1417541 - - - - - -
LEDA1439867 - 15 - 70 ± 6 - -
LEDA1446233 - - - - - -
LEDA1452135 - - - - - -
LEDA1464874 7 - 70 ± 17 - - -
LEDA3091160 44 8 100 ± 7 80 ± 18 - -
LEDA3127469 39 - 40 ± 5 - - -
LEDA3530 164 23 72 ± 1.1 90 ± 3 0.1 ± 0.04 -
LEDA49155 - 8 - 100 ± 17 - -
MCG+00-34-035 - - - - - -
NGC7401 13 - 80 ± 10 - - -
NGC99 30 - 60 ± 5 - - -
SDSSJ002048.58+141327.8 86 13 118 ± 1.5 120 ± 5 - -
SDSSJ011437.36+011053.4 - - - - - -
SDSSJ120108.03+152353.6 - - - - - -
SDSSJ135906.39+175604.9 - 11 - 110 ± 11 - -
SDSSJ140317.75+100340.3 81 25 60 ± 4 70 ± 2 - -
UGC10005 - - - - - -
UGC11992 - - - - - -
UGC272 7 - < 60 - - -
UGC6838 25 - 100 ± 5 - - -
UGC9359 - - - - - -
Z38-48 37 4 80 ± 3 100 ± 40 - -
Z383-30 25 - 60 ± 6 - - -
Z386-19 25 - 60 ± 5 - - -
Z429-16 90 22 80 ± 1.5 90 ± 4 0.3 ± 0.11 -
Z429-21 50 6 80 ± 2 < 110 - -
Z436-34 22 - 60 ± 6 - - -
Z68-62 17 5 70 ± 7 100 ± 40 - -
Z72-15 14 - 70 ± 9 - - -
Z80-42 35 6 70 ± 4 80 ± 16 - -
Z97-38 - - - - - -

LEDA1389480 41 11 70 ± 3 70 ± 5 - -
NGC2741 530 - 81 ± 1.1 - - -
MRK802 720 - 79 ± 0.6 - 0.31 ± 0.015 -
LEDA213877 - - - - - -
MRK444 510 40 102 ± 0.7 103 ± 0.8 0.12 ± 0.019 < 0.5
Z102-75 24 - 100 ± 3 - - -
NGC2607 4 4 20 ± 13 50 ± 20 - -
MRK399 229 26 118 ± 0.8 122 ± 1.3 - < 0.4
LEDA31379 17 - 100 ± 5 - 0.4 ± 0.12 -
MRK58 159 4 88 ± 0.9 130 ± 19 0.2 ± 0.04 -
LEDA3998175 - - - - - -
Z65-27 88 32 80 ± 1.6 114 ± 1.7 0.4 ± 0.06 0.4 ± 0.16
UGC7017 104 5 140 ± 1.5 110 ± 17 0.2 ± 0.08 -
LEDA86470 160 17 86 ± 0.7 110 ± 3 0.2 ± 0.07 -

Notes. Columns two and three list the emission line FWHM (deconvolved from instrumental resolution) for Hα and [OIII] derived from the single-component fit to the high-resolution spectroscopy where the fit was successful. Columns four and five show the ratio of flux in outflow-like fit components to the total flux in the emission line derived from the multi-component fit to the high-resolution spectroscopy for galaxies in which the best-fit model has outflow-like components (see Section 5.4). Galaxies in the upper section of the table were observed with NTT/EFOSC2 and those in the lower part with TNG/DOLORES.

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