Abstract

We report the detection of steady radio emission from the known X-ray source X9 in the globular cluster 47 Tuc. With a double-peaked C IV emission line in its ultraviolet spectrum providing a clear signature of accretion, this source had been previously classified as a cataclysmic variable. In deep ATCA imaging from 2010 and 2013, we identified a steady radio source at both 5.5 and 9.0 GHz, with a radio spectral index (defined as $S_{\nu}\propto\nu^{\alpha}$) of $\alpha=-0.4\pm0.4$. Our measured flux density of $42\pm4$ microJy/beam at 5.5 GHz implies a radio luminosity ($\nu L_{\nu}$) of 5.8e27 erg/s, significantly higher than any previous radio detection of an accreting white dwarf. Transitional millisecond pulsars, which have the highest radio-to-X-ray flux ratios among accreting neutron stars (still a factor of a few below accreting black holes at the same X-ray luminosity), show distinctly different patterns of X-ray and radio variability than X9. When combined with archival X-ray measurements, our radio detection places 47 Tuc X9 very close to the radio/X-ray correlation for accreting black holes, and we explore the possibility that this source is instead a quiescent stellar-mass black hole X-ray binary. The nature of the donor star is uncertain; although the luminosity of the optical counterpart is consistent with a low-mass main sequence donor star, the mass transfer rate required to produce the high quiescent X-ray luminosity of 1e33 erg/s suggests the system may instead be ultracompact, with an orbital period of order 25 minutes. This is the fourth quiescent black hole candidate discovered to date in a Galactic globular cluster, and the only one with a confirmed accretion signature from its optical/ultraviolet spectrum.

Highlights

  • Globular clusters (GCs) are extremely efficient at producing lowmass X-ray binaries (LMXBs), with a specific frequency over two orders of magnitude higher than that seen in the field (Clark 1975)

  • The most massive stars in a newly formed GC should collapse into black holes (BHs) within the first few Myr, and it was originally thought that following mass segregation (Spitzer 1969), mutual gravitational interactions would lead to the expulsion of almost all of these BHs (Kulkarni, Hut & McMillan 1993; Sigurdsson & Hernquist 1993; Portegies Zwart & McMillan 2000)

  • Assuming that they are not ejected at formation, the BHs will rapidly segregate to the cluster centre, and the exchange of energy between the BH subcluster and the rest of the stars in the cluster allows a significant fraction of the BHs to be retained up to the present day

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Summary

Introduction

Globular clusters (GCs) are extremely efficient at producing lowmass X-ray binaries (LMXBs), with a specific frequency over two orders of magnitude higher than that seen in the field (Clark 1975). Once the BH population has been sufficiently depleted the BHs cannot provide sufficient energy to the rest of the cluster, which enters a phase of ‘core collapse’ (defined observationally via a steep radial density profile in the central regions), leading to the rapid ejection of the remaining BHs (Breen & Heggie 2013; Heggie & Giersz 2014).

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