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Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

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of the reduced spectrum for each slit position observed on each galaxy, along with<br />

(ii) Gaussian l<strong>in</strong>e fits to the same (see §4.1).<br />

3.3 Analysis<br />

In this section we describe the l<strong>in</strong>e fitt<strong>in</strong>g that we carried out on each spectral row<br />

of each reduced CCD spectral image, firstly with a s<strong>in</strong>gle Gaussian per spectral l<strong>in</strong>e<br />

(§4.1) <strong>and</strong> secondly with the <strong>in</strong>clusion of an additional free component (§4.2). In<br />

§4.3 we discuss the sizes of the errors on quoted parameters from various sources. In<br />

§4.4 we describe each of the UGC FR-I sample members <strong>in</strong> turn. For each galaxy<br />

we def<strong>in</strong>e the central spectrum as the row with the greatest <strong>in</strong>tegrated flux after the<br />

data reduction. We list the row numbers <strong>in</strong> the f<strong>in</strong>al x2d image correspond<strong>in</strong>g to the<br />

central spectrum <strong>in</strong> Table 3.1.<br />

3.3.1 S<strong>in</strong>gle Gaussian l<strong>in</strong>e fitt<strong>in</strong>g<br />

In the G750M spectra we expect to f<strong>in</strong>d the emission l<strong>in</strong>es <strong>in</strong> the vic<strong>in</strong>ity of Hα that are<br />

listed <strong>in</strong> Table 3.4. We used wavelengths from the recent measurements of Wallerste<strong>in</strong><br />

et al. (2001) <strong>and</strong> converted from air to vacuum wavelengths us<strong>in</strong>g the IAU st<strong>and</strong>ard<br />

formula<br />

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