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Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

Gas Disks and Supermassive Black Holes in Nearby Radio Galaxies

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<strong>Gas</strong> Radial Velocity (km s -1 )<br />

<strong>Gas</strong> Radial Velocity (km s -1 )<br />

<strong>Gas</strong> Radial Velocity (km s -1 )<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

NGC383 Central Slit: ∆v = 120 km s -1<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

-ve offset slit position<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

+ve offset slit position<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

<strong>Gas</strong> Radial Velocity (km s -1 )<br />

<strong>Gas</strong> Radial Velocity (km s -1 )<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

NGC383 Central Slit: ∆v = 220 km s -1<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

-ve offset slit position<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

+ve offset slit position<br />

-0.4 -0.2 0.0 0.2 0.4<br />

Position along slit (arcsec)<br />

Figure 4.25 The observed velocity profiles of NGC 383 for each of the three observed<br />

slit positions: (left) offset by the velocity <strong>and</strong> slope calculated <strong>in</strong> §4.2.5 <strong>and</strong> (right)<br />

with a velocity offset of 220 km s −1 , which provides a more mean<strong>in</strong>gful fit (judged<br />

by the author), extra power <strong>in</strong> the velocity field <strong>in</strong> the side slit position may result<br />

from the nucleus ly<strong>in</strong>g off center across the width of the central slit. The velocities<br />

are shown shaded accord<strong>in</strong>g to the relative signal-to-noise of each spectrum, formal<br />

errors from the fit are also <strong>in</strong>dicated (see Chapter 3). The three solid l<strong>in</strong>es show<br />

model velocity profiles for no black hole, a 1 × 10 8 M⊙ black hole <strong>and</strong> a 9 × 10 8 M⊙<br />

(the steeper l<strong>in</strong>es from models with the greatest black hole mass). See text for details<br />

of the models. The dashed vertical l<strong>in</strong>es give a rough approximation of the radius of<br />

<strong>in</strong>fluence of a black hole based on the mass estimate from the M• − σ relation <strong>and</strong><br />

the size of the r<strong>and</strong>om motions observed.<br />

<strong>Gas</strong> Radial Velocity (km s -1 )<br />

200<br />

0<br />

-200<br />

-400<br />

-600<br />

212

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