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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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NGC 5141: This S0 galaxy has a nuclear dust lane. The STIS slits were aligned<br />

parallel to the galaxy major axis, 16 ◦ from the dust axis. The weighted mean obser-<br />

vation - model residuals are plotted <strong>in</strong> Figure 4.14 <strong>and</strong> gives a m<strong>in</strong>imum at an offset<br />

of −50 km s −1 , equivalent to a galaxy recessional velocity of 5253 km s −1 . The model<br />

velocity profiles for these observations are shown <strong>in</strong> Figure 4.37. The gas velocities<br />

are very well settled <strong>in</strong>to a smooth rotation curve, however no nuclear black hole is<br />

necessary to expla<strong>in</strong> the observed k<strong>in</strong>ematics.<br />

NGC 5490: This elliptical galaxy has a nuclear dust lane. The STIS slits were<br />

aligned parallel to the galaxy major axis, 43 ◦ from the dust disk axis. The weighted<br />

mean observation - model residuals are plotted <strong>in</strong> Figure 4.15 <strong>and</strong> gives a m<strong>in</strong>imum<br />

at an offset of −93 km s −1 , equivalent to a galaxy recessional velocity of 5697 km s −1 .<br />

The model velocity profiles for these observations are shown <strong>in</strong> Figure 4.38. It is not<br />

clear that the modeled velocity profiles match any of the observed k<strong>in</strong>ematics <strong>in</strong> the<br />

nuclear region. The fact that the dust disk <strong>and</strong> galaxy major axis are not co<strong>in</strong>cident<br />

by a sizeable angle also means that it is not clear what plane the gas will lie <strong>in</strong>, images<br />

of the emission l<strong>in</strong>e disks (Verdoes Kleijn et al., 1999) do not make this any clearer.<br />

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