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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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gas disks were computed by mak<strong>in</strong>g a circular th<strong>in</strong> disk assumption <strong>and</strong> deriv<strong>in</strong>g<br />

the <strong>in</strong>cl<strong>in</strong>ation angle from the observed axis ratio of the dust. For the galaxies with<br />

dust lanes, <strong>in</strong>cl<strong>in</strong>ations were set at 80 ◦ (we do not observe disks below about 70 ◦ ,<br />

which we <strong>in</strong>terpret of the lower limit of the range of <strong>in</strong>cl<strong>in</strong>ations <strong>in</strong> systems where we<br />

see lanes). The measured axis ratios <strong>and</strong> derived <strong>in</strong>cl<strong>in</strong>ations are given <strong>in</strong> Table 4.1,<br />

along with dust masses.<br />

4.2.2 Flux distributions<br />

To model the observed gas k<strong>in</strong>ematics we first need a description of the <strong>in</strong>tr<strong>in</strong>sic<br />

emission l<strong>in</strong>e flux distribution, for which we make use of the flux profiles obta<strong>in</strong>ed<br />

from the Gaussian fits to our STIS spectroscopic results that we presented <strong>in</strong> Chapter<br />

3, Tables 3.5 to 3.25. We model the face on flux profile as a double exponential,<br />

151<br />

F(R) = F1e −R/R1 + F2e −R/R2 , (4.1)<br />

deriv<strong>in</strong>g the parameters assum<strong>in</strong>g an <strong>in</strong>f<strong>in</strong>itesimally th<strong>in</strong> disk, <strong>in</strong>cl<strong>in</strong>ed at the angle<br />

given <strong>in</strong> Table 4.1. We iterate a fit of the double exponential to the flux data, tak<strong>in</strong>g<br />

<strong>in</strong>to account the flux errors <strong>and</strong> convolution with the STIS PSF, aperture size <strong>and</strong><br />

pixel size.<br />

The STIS PSF was represented by a comb<strong>in</strong>ation of five Gaussians which represent

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