The spin of the black hole microquasar XTE J1550−564 via the continuum-fitting and Fe-line methods

We measure the spin of XTE J1550−564 using the two leading methods: (i) modelling the thermal continuum spectrum of the accretion disc; and (ii) modelling the broad red wing of the reflection fluorescence Fe Kα line. We find that these two independent measurements of spin are in agreement. For the c...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2011-09, Vol.416 (2), p.941-958
Hauptverfasser: Steiner, James F., Reis, Rubens C., McClintock, Jeffrey E., Narayan, Ramesh, Remillard, Ronald A., Orosz, Jerome A., Gou, Lijun, Fabian, Andrew C., Torres, Manuel A. P.
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Sprache:eng
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Zusammenfassung:We measure the spin of XTE J1550−564 using the two leading methods: (i) modelling the thermal continuum spectrum of the accretion disc; and (ii) modelling the broad red wing of the reflection fluorescence Fe Kα line. We find that these two independent measurements of spin are in agreement. For the continuum-fitting analysis, we use a data sample consisting of several dozen Rossi X-ray Timing Explorer spectra, and for the Fe Kα analysis, we use a pair of ASCA spectra from a single epoch. Our spin estimate for the black hole primary using the continuum-fitting method is −0.11 < a * < 0.71 (90 per cent confidence), with a most likely spin of a *= 0.34. In obtaining this result, we have thoroughly explored the dependence of the spin value on a wide range of model-dependent systematic errors and observational errors; our precision is limited by uncertainties in the distance and orbital inclination of the system. For the Fe-line method, our estimate of spin is a *= 0.55+0.15 − 0.22. Combining these results, we conclude that the spin of this black hole is moderate, a *= 0.49+0.13 − 0.20, which suggests that the jet activity of this microquasar is powered largely by its accretion disc rather than by the spin energy of the black hole.
ISSN:0035-8711
1365-2966
DOI:10.1111/j.1365-2966.2011.19089.x