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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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1.1 <strong>Radio</strong> galaxies<br />

A radio galaxy can produce a jet-lobe, radio wavelength emitt<strong>in</strong>g, structure on mega-<br />

parsec scales, emerg<strong>in</strong>g from a central eng<strong>in</strong>e that resides <strong>in</strong> an active region no more<br />

than a few milli-parsecs <strong>in</strong> size. The radio emission is well understood to be from<br />

synchrotron radiation, but the processes <strong>in</strong>volved <strong>in</strong> fuel<strong>in</strong>g <strong>and</strong> collimat<strong>in</strong>g the ra-<br />

dio jets are yet to be expla<strong>in</strong>ed (Lynden-Bell, 2001). The energy that powers the<br />

radio jets is typically believed to be produced dur<strong>in</strong>g the accretion of material onto<br />

a central supermassive black hole (e.g., Lynden-Bell, 1969). The formation of such<br />

well organized large scale jet structures is some of the most compell<strong>in</strong>g evidence for<br />

the necessity of supermassive black holes as an <strong>in</strong>gredient <strong>in</strong> the makeup of a radio<br />

galaxy (Rees, 1984).<br />

<strong>Radio</strong> emission can be detected even from relatively quiescent galaxies, such<br />

as the Milky Way, on the level of around 10 37 erg s −1 . Active galaxies (such as<br />

Seyferts or starburst galaxies) radiate at around 10 37 erg s −1 , <strong>and</strong> radio galaxies (<strong>and</strong><br />

also quasars) extend this energy output range to beyond 10 45 erg s −1 (∼ 10 12 L⊙)<br />

(Burke & Graham-Smith, 1997). An active galaxy central eng<strong>in</strong>e capable of releas-<br />

<strong>in</strong>g ∼ 0.1Mfuelc 2 of <strong>in</strong>fall<strong>in</strong>g fuel as radiation would need to be fueled at a rate of<br />

∼> 1 M⊙ yr −1 to ma<strong>in</strong>ta<strong>in</strong> this lum<strong>in</strong>osity.<br />

3

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