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Table 3.

Main kinematical parameters derived from the stellar modelling and for the individual components detected in the gas modelling of the Hα line for all the cubes.

Galaxy PA Δv PAgas, P Δvgas, P vgas, S Broad FWHM
(°) (km s−1) (km s−1) (°) (km s−1) (km s−1) (km s−1) (km s−1) (Y or N) (km s−1)
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11)
NGC 0266 121 ± 7 172 182 ± 14 173 ± 28 N
NGC 0315 335 ± 13 225 ± 8 156 195 ± 38 96 ± 77 480 ± 120 Y 2655 ± 360
NGC 3226 49 ± 4 106 210 ± 17 19 ± 4 219 136 ± 55 −91±27 262 ± 42 Y 2305 ± 153
NGC 3245 178 ± 3 144 245 ± 18 174 ± 6 232 154 ± 46 −214 ± 142 198 ± 173 N
NGC 4278( † ) 20 ± 1 104 336 ± 35 46 ± 10 240 146 ± 23 82 ± 150 49 ± 27
NGC 4438 27 ± 2 111 148 ± 7 28 ± 6 154 99 ± 28 −8 ± 35 256 ± 57 [Y] [1980 ± 350]
NGC 4750 210 ± 10 97 134 ± 7 153 ± 29 −92 ± 50 297 ± 41 Y 2188 ± 300
NGC 5055 99 ± 4 79 50 ± 4 107 ± 11 126 69 ± 26 N

Notes. Columns indicate: (1) object, ( † )indicates that the values correspond to the [O III] line; (2) major axis position angle of the stellar velocity maps using the receding sides as reference; (3) semi-amplitude velocity of the stellar maps; (4) central velocity dispersion in the PSF region of the stellar maps; (5) position angle for the major axis of the primary component of the ionised gas; (6) and (7) semi-amplitude velocity and central velocity dispersion (in the PSF region) of the primary component of the ionised gas; (8) and (9) average velocity and velocity dispersion integrated in the PSF region for the secondary component of the ionised gas; (10) indicates if there is or not a broad component associated with the BLR detected in the Balmer lines and (11) the FWHM of that component. For all columns, the reported errors are 1σ values. [] indicates that the BLR fit is not well constrained.

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