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observational overview of state transitions in x-ray binaries

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No Compact Jet<br />

(<strong>in</strong>teraction with<br />

ISM)<br />

Fender, Belloni, Gallo 2004<br />

Fender, Homan, Belloni, 2009<br />

s<strong>of</strong>t<br />

Ejection<br />

Events<br />

rms-drop<br />

type-B QPOs<br />

JETS<br />

Compact<br />

Jet Switches on<br />

(radio)<br />

Radio<br />

Flare<br />

hard<br />

Compact<br />

Jet Weakens<br />

(radio/nIR)<br />

Compact<br />

Jet<br />

Compact<br />

Jet Switches on<br />

(nIR)<br />

Homan et al. 2005<br />

Russell et al. 2006<br />

Coriat et al. 2009<br />

I’m go<strong>in</strong>g to use the same schematic aga<strong>in</strong> and will summarize the picture that is emerg<strong>in</strong>g<br />

from various radio and nIR papers. I’ll start with the hard <strong>state</strong> and progress through the<br />

diagram <strong>in</strong> an anti-clockwise manner. The hard <strong>state</strong> gives rise to steady radio emission from<br />

a compact jet. Radio and nIR emission scale <strong>in</strong> similar ways with the X-<strong>ray</strong> lum<strong>in</strong>osity. Once a<br />

system turns the corner the radio and nIR start to weaken, suggest<strong>in</strong>g the jet is gett<strong>in</strong>g less<br />

powerful. Than at some po<strong>in</strong>t dur<strong>in</strong>g the transition a radio flare is observed, which is thought<br />

to be the result <strong>of</strong> an ejection event. Interest<strong>in</strong>gly, this flare always seems to take place with<strong>in</strong><br />

a few days <strong>of</strong> this zone with odd variability properties that I just discussed. In sources that<br />

cross this zone multple times dur<strong>in</strong>g an outburst, like XTE J1858+226, we see radio flares<br />

associated with rms drops <strong>in</strong> all cases. Bright sources that enter the steep power law <strong>state</strong><br />

suggest that ejection events cont<strong>in</strong>ue to occur <strong>in</strong> that <strong>state</strong>.<br />

No radio emission from the central source is seen <strong>in</strong> the s<strong>of</strong>t <strong>state</strong>. If there is radio emission it<br />

is likely the result <strong>of</strong> <strong>in</strong>teraction <strong>of</strong> the jet ejecta with the ISM.<br />

At some po<strong>in</strong>t the source starts it return to the hard <strong>state</strong>. We’re not exactly sure when the<br />

jet switches on aga<strong>in</strong> <strong>in</strong> the radio, but from at least one source it is clear that it start<br />

somewhere halfway <strong>in</strong> the transition, and perhaps even earlier. In the near-<strong>in</strong>frared jet<br />

emission only becomes significant when it reaches the hard <strong>state</strong>.

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