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Table 2:

Derived parameters for the profile width sub-sample.
ID $\alpha_{2000}$ $\delta_{2000}$ $V_{\rm sys}$ D MV (V-I) $M_{\rm HI}$ W20 W50 W20 $_{\rm {,~turb}}$ W50 $_{\rm {,~turb}}$ i
  (h m s) ( $\circ~~~ \hbox{$^\prime$ }~~~ \hbox{$^{\prime\prime}$ }$)  km s-1 Mpc mag   107 $M_{\odot}$  km s-1  km s-1  km s-1  km s-1 $^\circ$
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13)
D572-5 11 48 16.4 +18 38 33 994 14.6 -14.56 0.52 8.55 77 62 68 55 50a
D575-1 12 51 46.1 +21 44 07 600 10.0 -14.22 0.70 3.76 38 24 30 18 53
D575-5 12 55 41.4 +19 12 34 437 7.7 -13.21 0.44 4.27 28 19 16 10 50
D640-13 10 56 13.9 +12 00 41 958 13.4 -14.36 0.55 4.53 38 25 30 18 48a
D646-7 12 58 40.4 +14 13 03 233 2.1b -12.52 0.84 0.37 35 23 26 16 55a
a Optical I-band inclination from Pildis et al. (1997).
b Distance as given in Karachentsev et al. (2003).
Notes: (1) galaxy identifier; (2, 3) central position taken from NED; (4) systemic velocity derived from the central velocity of the W50 profile; (5) distance in Mpc. If no reference is given, the distance is based on $V_{\rm sys}$(Col. 4) and a Hubble flow using $H_0=75\rm {~{km}~{s}^{-1}~Mpc^{-1}}$, including a correction for Virgocentric infall (Mould et al. 2000); (6) absolute V-band magnitude as given in Pildis et al. (1997), corrected to our distance estimates; (7) V-I color from Pildis et al. (1997); (8) total H  I mass (in units of $10^7~M_{\odot}$); (9) uncorrected width of the H  I profile at the 20 percent level of the maximum intensity. The values listed here for W20 are derived using the Hanning smoothed data; (10) as Col. 9, but for the W50 profile; (11) width of the W20 profile, corrected for the finite velocity resolution, and turbulent motion of the H  I gas; (12) as Col. 11, but for the W50 profile; (13) adopted inclination angle. The velocity widths in Cols. (9)-(12) are not corrected for inclination effects.

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