We discuss the evolution of black hole transients on the basis of a few systems that were intensively observed with the Rossi X-ray Timing Explorer. We focus on the global evolution and the observed state transitions. Rather than giving a numerical recipe
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4.2.Thehardstate softstatetransitions
Immediatelyafterleavingandbeforereturningtothehardstate,blackholetransientsareobservedinanintermediatestate,withspectralpower-lawindicesbetweenroughly1.5–2.5.Wearenotawareofanyexceptiontothis.Thisstateisdi erentfromthehardstateinsev-eralaspects.Dependingonwhethertheintermediatestateisobservedduringthehard→softorsoft→hardtransition,sourcesshowaclearsteepening/ atteningofthespectralpowerlawcomponent,astrongincrease/decreaseinthenoiseandQPOfrequencies,andanincreas-ing/decreasingfractionaldisk ux,comparedtothehardstate.Allthesepropertiesevolvesmoothlyfromandtothehardstate.Infact,withouttheHIDandoptical/IRinformation(seeFig.4)itwouldbedi culttoexactlypin-pointthetransitionbetweenthesetwostates.Inthecaseofthehard→softtransitionthemovementtotheleftintheHIDisduetothecombinationofincreaseddisk uxandsteepeningofthepowerlaw.Inthetimingdomain,thebroad-bandvariabilitycomponentsseeninthepowerdensityspectrumincreasetheirchar-acteristicfrequencies,showinganevolutionthatclearlylinksthemtothecorrespondingcomponentsinthehardstate.AcleartypeCQPOappears,alsowithacharacteristicfrequencyincreasingwithtimeanddecreasinghardness(seeBellonietal.(2004)).Atypicalpower-densityspectrumfromtheintermediatestateisshowninFigure3.
Itisimportanttonotethatthehard→intermediatestatetransitiondoesnotalwaysoccuratthesame uxlevel,ascanbeseenfromFigure
4.Duringthe2004outburstofGX339–4thistransitionoccurredata uxlevelthatwasaboutafactorof4lowerthanin2002.Thetransitionin2004wasprecededbyasmallhardstateoutburst,whichsuggeststhatthe uxlevelatwhichthetransitionoccursdependsontherecentaccretionhistory.AfterpassingthroughtheintermediateGX339-4continuedtobrighteninthesoftsateduringits2004outburst.
Anotherimportantpointtonoteisthefactthattheoccurrenceoftheintermediatestatedoesnotseemtodependonthetimederivative˙.InXTEJ1650–500itoccurredduringthedecay,butinGX339–ofM˙wasapparentlystillincreasing,aswitnessedbythesecond4whileM(soft)maximuminthelightcurve.However,inbothcasesthetransitionresultedina(temporary)dropinthecountratebyafactorof~2.Takingoncemorethe2002/2003outburstofGX339–4asatem-plate,weseethatwhenthehardnessgoesbelowawellde nedthresh-old,thetimingpropertieschangesharply:acleartypeBQPOappearsinthepowerdensityspectrum(Figure3,seealsoCasellaetal.,2004forsimilarbehaviorinXTEJ1859+226).InmostsourcesthechangefromtypeCtotypeBQPOsseemstotakeplacewhenthepower-law
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