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Table 1.

Observation: Properties of GN4_32842.

z abar Re vc(Re) σ0 log ( M b M ) $ \log\left(\frac{M_{\mathrm{b}}}{M_\odot}\right) $ B/T SFR fDM(< Re) fgas Qgas vr(in-plane) δvr v r ( in-plane ) v r ( Toomre ) $ \frac{v_{\mathrm{r}}(\text{ in-plane})}{v_{\mathrm{r}}(\text{ Toomre})} $ δ v r ( in-plane ) v r ( Toomre ) $ \delta\frac{v_{\mathrm{r}}(\text{ in-plane})}{v_{\mathrm{r}}(\text{ Toomre})} $
[kpc] [kpc] [km/s] [km/s] [M/yr] [km/s] [km/s]
1.52 4.5 7.5 379 48 11.30 0.09 106.6 0.5 0.26 0.69 60 13 2.7 0.9

Notes. Redshift (column 1), deprojected semimajor axis of the bar (column 2), effective radius of the disk and the circular velocity at it (columns 3 and 4), velocity dispersion (column 5), logarithm of the total baryonic mass and bulge to total ratio (columns 6 and 7), SFR (column 8), inner dark matter fraction within Re (column 9), gas fraction (column 10), gas Toomre Q stability parameter (column 11), estimated amplitude of in-plane radial motions computed as vr(in-plane) = vresid/sin i and its uncertainty (columns 12 and 13), and the ratio of the in-plane radial over the Toomre velocity with its respective uncertainty (columns 14 and 15).

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