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Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

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Difference <strong>in</strong> mean velocity on each side of nucleus (km s -1 )<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

0<br />

0.0 0.2 0.4 0.6 0.8 1.0<br />

Axis Ratio (b/a or width:length)<br />

Figure 3.24 Difference <strong>in</strong> mean velocity with<strong>in</strong> 100 pc of each side of the nucleus<br />

(∆100pc, see text) as a function of dust disk axis ratio (b/a) or dust lane width : length<br />

ratio, which is an <strong>in</strong>dicator of <strong>in</strong>cl<strong>in</strong>ation. The different k<strong>in</strong>ematic classes <strong>and</strong> dust<br />

morphologies are <strong>in</strong>dicated. Filled symbols represent rotators: with dust disks (•),<br />

with dust lanes (�) or with irregular dust (�); Empty symbols represent non-rotators:<br />

with dust disks (◦), with dust lanes (�) or with no-dust or irregular dust (△). The<br />

solid l<strong>in</strong>es are loci for disks with the same <strong>in</strong>tr<strong>in</strong>sic ∆100pc (990, 680 <strong>and</strong> 360 km s −1 )<br />

viewed at <strong>in</strong>cl<strong>in</strong>ations projected assum<strong>in</strong>g b/a = s<strong>in</strong> i (i.e. a circular disk).<br />

144

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