The spin of the black hole microquasar XTE J1550−564 via the continuum-fitting and Fe-line methods
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Author
Steiner, James F.
Reis, Rubens C.
Remillard, Ronald A.
Orosz, Jerome A.
Gou, Lijun
Fabian, Andrew C.
Torres, Manuel A. P.
Published Version
https://doi.org/10.1111/j.1365-2966.2011.19089.xMetadata
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Steiner, James F., Rubens C. Reis, Jeffrey E. McClintock, Ramesh Narayan, Ronald A. Remillard, Jerome A. Orosz, Lijun Gou, Andrew C. Fabian, and Manuel A. P. Torres. 2011. “The Spin of the Black Hole Microquasar XTE J1550−564 via the Continuum-Fitting and Fe-Line Methods.” Monthly Notices of the Royal Astronomical Society 416, no. 2: 941–958.Abstract
We measure the spin of XTE J1550-564 in two ways: by modelling the thermal continuum spectrum of the accretion disc, and independently by modeling the broad red wing of the reflection fluorescence Fe-K line. We find that the spin measurements conducted independently using both leading methods are in agreement with one another. For the continuum-fitting analysis, we use a data sample consisting of several dozen RXTE spectra, and for the Fe-K 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 of this microquasar is powered largely by its accretion disc rather than by the spin energy of the black hole.Other Sources
http://arxiv.org/pdf/1010.1013v2.pdfTerms of Use
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