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Table 4:

Gas kinematic results.
Galaxy $cz_{{\rm nuc, H}\alpha}$ $\Delta v_{{\rm H}\alpha}$ $\sigma_{{\rm nuc, H}\alpha}$
(1) (2) (3) (4)
NGC 23 $4495\pm 9$ -215, +236 $139\pm 17$
MCG +12-02-001 $4732\pm 8$ -110, +156 $105\pm 14$
UGC 1845 $4796\pm 9$ -237, +181 $142\pm 17$
NGC 2388 $4093\pm 9$ -157, +163 $115\pm 15$
MCG +02-20-003 $4950\pm 9$ -141, +110 $96\pm 13$
IC 860* $4146\pm 13$ $\cdots$ $\cdots$
NGC 5936 $3984\pm 13$ -66, +179 $66\pm 15$
NGC 6701 $3946\pm 13$ -41, +102 $92\pm 16$
NGC 7469 $4946\pm 9^{**}$ -110,+207** $125\pm 16^{**}$
NGC 7591 $4869\pm 9$ -179, +345 $144 \pm 17$
NGC 7771 $4334\pm 9$ -181, +199 $106\pm 14$

Notes. - Column (2): $cz_{{\rm nuc, H}\alpha}$ is the H$\alpha $ velocity of the nucleus, defined as the peak of the 6200 Å continuum, except for NGC 7771 where it is refered to the position that makes the velocity field gradient symmetric (see text and Fig. 3c). Column (3): $\Delta v_{{\rm H}\alpha}$ is the H$\alpha $peak-to-peak velocity range over the PMAS FoV. Column (4): $\sigma_{{\rm nuc, H}\alpha}$ is the nuclear H$\alpha $ velocity dispersion (corrected for instrumental effects). All measurements are in km s-1, and are not corrected for inclination and/or angular resolution effects; * for IC 860 $cz_{\rm nuc}$ is from [N  II]$\lambda $6584 and [S  II] $\lambda \lambda $6717,6731. We note that NED quotes a value of $3347~{\rm km~s}^{-1}$ from 21 cm H  I measurements, whereas our value of the velocity is confirmed by measurements of the mid-infrared emission lines with Spitzer/IRS (Pereira-Santaella et al. 2005, in preparation); ** for NGC 7469 the measurements are from [N  II]$\lambda $6584.


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