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observational overview of state transitions in x-ray binaries

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STEEP POWER-LAW STATE<br />

radio ejections<br />

F<strong>in</strong>ally there’s the steep power-law <strong>state</strong>. In light curve this <strong>state</strong> is characterized by very<br />

strong flar<strong>in</strong>g on a time scale <strong>of</strong> days. This <strong>state</strong> is only observed at the very highest<br />

lum<strong>in</strong>osities. The spectrum <strong>of</strong> this <strong>state</strong> is dom<strong>in</strong>ated by a steep power -law component on<br />

top <strong>of</strong> a very hot accretion disk component. Aga<strong>in</strong>, the non-thermal component is poorly<br />

understood, but is is probably the results <strong>of</strong> <strong>in</strong>verse Compton scatter<strong>in</strong>g.<br />

We see many different types <strong>of</strong> power spectra and they seem to comb<strong>in</strong>e elements <strong>of</strong> power<br />

spectra seen <strong>in</strong> the other <strong>state</strong>s, with different types <strong>of</strong> noise and QPOs. In the radio with<br />

<strong>of</strong>ten see optically th<strong>in</strong> ejection events.<br />

In a way it is quite similar to the <strong>in</strong>termediate <strong>state</strong>, with a hotter disk and the power-law<br />

chang<strong>in</strong>g <strong>in</strong> normalization rather than <strong>in</strong>dex. It has been suggested that this <strong>state</strong><br />

corresponds to the presence <strong>of</strong> a thickened or slim disk.

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