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.

Highlights

  • During its principal 1998–1999 outburst cycle, the bright Xray transient XTE J1550–564 produced one of the most remarkable flare events ever observed for a black hole binary

  • The Spin of the Black Hole in XTE J1550–564 3 considered in their study, and additional data; unlike this exploratory and preliminary study of eight blackhole systems, we fixedly focus on J1550 and so are able to refine and improve upon their work

  • In selecting our data and for determining the spin, we employ a variant of the principal model that we used in our earlier study of J1550 and H1743–322: crabcor×tbabs×smedge(simpl⊗kerrbb2)

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Summary

Introduction

During its principal 1998–1999 outburst cycle, the bright Xray transient XTE J1550–564 produced one of the most remarkable flare events ever observed for a black hole binary. For ≈ 1 day, the source intensity rose fourfold relative to neighbouring plateau values, reaching 6.8 Crab. The flux in the dominant power-law component rose by the same factor, and just as quickly its intensity declined (Sobczak et al 2000; McClintock et al 2009). AU-scale superluminal radio jets were observed (Hannikainen et al 2009). Their separation angle (∼ 255 mas) and relative velocity (∼ 65 mas d−1) links the birth of these jets to the impulsive X-ray flare.

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