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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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models. Pronounced differences can be produced by differences <strong>in</strong> the angle of the<br />

slits compared to the k<strong>in</strong>ematic major axis of the gas. This may pose problems <strong>in</strong><br />

morphologically complex systems where we have no way of a priori determ<strong>in</strong><strong>in</strong>g the<br />

k<strong>in</strong>ematic axes.<br />

4.3 Descriptions of <strong>in</strong>dividual galaxies<br />

For each galaxy we compare the three models we obta<strong>in</strong>ed for 0, 1 × 10 8 M⊙ <strong>and</strong><br />

9 × 10 8 M⊙ black holes to the observed velocities <strong>in</strong> all three slits. We do not model<br />

UGC 7115 (where we only have one spectroscopic slit, <strong>and</strong> relatively low signal to<br />

noise), nor NGC 3801 (where we are clearly not on the nucleus <strong>and</strong> not aligned with<br />

the k<strong>in</strong>ematic axis). We present the results <strong>in</strong> Figures 4.23 to 4.41 <strong>and</strong> describe each<br />

galaxy <strong>in</strong> turn below.<br />

NGC 193: This S0 galaxy has a complex dust morphology with two dist<strong>in</strong>ct dust<br />

systems clearly visible. The STIS slits were aligned parallel to the galaxy major axis,<br />

which is also almost perpendicular to the radio jets. The weighted mean observation<br />

- model residuals are plotted <strong>in</strong> Figure 4.1 <strong>and</strong> gives a m<strong>in</strong>imum at an offset of<br />

47 km s −1 , equivalent to a galaxy recessional velocity of 4390 km s −1 . The model<br />

velocity profiles for these observations are shown <strong>in</strong> Figure 4.23, two plots are shown,<br />

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