Radio Detections During Two State Transitions of the Intermediate-Mass Black Hole HLX-1

Big Black Holes Black holes come in two sizes: stellar-mass black holes, with masses just above that of the Sun, and supermassive black holes, with masses up to a billion times that of the Sun. The hyperluminous x-ray source HLX-1 in the spiral galaxy ESO 243-49 is the best candidate to host a black hole of intermediate mass. Webb et al. (p. 554, published online 5 July) now report the detection of transient radio emission from this source, which may represent a jet ejection event. The radio flares indicate a mass that is consistent with that of an intermediate mass black hole. Jets have been seen to emanate from both supermassive and stellar-mass black holes. Intermediate mass black holes thus seem to behave like other black holes. Observations of a candidate intermediate-mass black hole support the scale invariance of jets in black holes. Relativistic jets are streams of plasma moving at appreciable fractions of the speed of light. They have been observed from stellar-mass black holes (~3 to 20 solar masses, M☉) as well as supermassive black holes (~106 to 109 M☉) found in the centers of most galaxies. Jets should also be produced by intermediate-mass black holes (~102 to 105 M☉), although evidence for this third class of black hole has, until recently, been weak. We report the detection of transient radio emission at the location of the intermediate-mass black hole candidate ESO 243-49 HLX-1, which is consistent with a discrete jet ejection event. These observations also allow us to refine the mass estimate of the black hole to be between ~9 × 103 M☉ and ~9 × 104 M☉.

[1]  Alan A. Wells,et al.  The Swift Gamma-Ray Burst Mission , 2004, astro-ph/0405233.

[2]  L. Zampieri,et al.  Low metallicity natal environments and black hole masses in Ultraluminous X-ray Sources , 2009, 0909.1017.

[3]  T. Belloni,et al.  A Unified Model for Black Hole X-Ray Binary Jets? , 2004, astro-ph/0506469.

[4]  A Fundamental plane of black hole activity , 2003, astro-ph/0305261.

[5]  Z. Paragi,et al.  BLACK HOLE POWERED NEBULAE AND A CASE STUDY OF THE ULTRALUMINOUS X-RAY SOURCE IC 342 X-1 , 2012, 1201.4473.

[6]  Didier Barret,et al.  An intermediate-mass black hole of over 500 solar masses in the galaxy ESO 243-49 , 2009, Nature.

[7]  H. Falcke,et al.  Refining the fundamental plane of accreting black holes , 2006, astro-ph/0603117.

[8]  Radio Emission Associated with the Ultraluminous X-Ray Source in Holmberg II , 2005 .

[9]  T. P. Roberts,et al.  The Ultraluminous State , 2009, 0905.4076.

[10]  P. Giommi,et al.  The Swift X-Ray Telescope , 1999 .

[11]  Roberto Soria,et al.  Discovery of an optical counterpart to the hyperluminous X-ray source in ESO 243-49 , 2009, 0910.1356.

[12]  N. Gehrels,et al.  FIRST EVIDENCE FOR SPECTRAL STATE TRANSITIONS IN THE ESO 243-49 HYPERLUMINOUS X-RAY SOURCE HLX-1 , 2009, 0909.4458.

[13]  R. P. Fender,et al.  Initial low/hard state, multiple jet ejections and X-ray/radio correlations during the outburst of XTE J1859+226 , 2001, astro-ph/0112137.

[14]  A. Tzioumis,et al.  On the Origin of Radio Emission in the X-Ray States of XTE J1650-500 during the 2001-2002 Outburst , 2004, astro-ph/0409154.

[15]  Philip Kaaret,et al.  Radio Emission from an Ultraluminous X-ray Source , 2003, Science.

[16]  M. Servillat,et al.  CHANDRA AND SWIFT FOLLOW-UP OBSERVATIONS OF THE INTERMEDIATE-MASS BLACK HOLE IN ESO 243-49 , 2010, 1002.3625.

[17]  John C. Geary,et al.  Kepler-36: A Pair of Planets with Neighboring Orbits and Dissimilar Densities , 2012, Science.

[18]  T. Belloni,et al.  Jets from black hole X-ray binaries: testing, refining and extending empirical models for the coupling to X-rays , 2009, 0903.5166.

[19]  India,et al.  The Australia Telescope Compact Array Broadband Backend (CABB): Description & First Results ⋆ , 2011, 1105.3532.

[20]  R. Sunyaev,et al.  The non-linear dependence of flux on black hole mass and accretion rate in core-dominated jets , 2003, astro-ph/0305252.

[21]  P. S. Bunclark,et al.  Astronomical Data Analysis Software and Systems , 2008 .

[22]  Didier Barret,et al.  A REDSHIFT FOR THE INTERMEDIATE-MASS BLACK HOLE CANDIDATE HLX-1: CONFIRMATION OF ITS ASSOCIATION WITH THE GALAXY ESO 243-49 , 2010, 1008.4125.

[24]  E. Colbert,et al.  Intermediate - mass black holes , 2003 .

[25]  Sera Markoff,et al.  Population X: Are the super-Eddington X-ray sources beamed jets in microblazars or intermediate mass black holes? , 2002 .

[26]  P. Madau,et al.  SIMULATIONS OF RECOILING MASSIVE BLACK HOLES IN THE VIA LACTEA HALO , 2009, 0907.0892.

[27]  M. Servillat,et al.  X-RAY VARIABILITY AND HARDNESS OF ESO 243–49 HLX-1: CLEAR EVIDENCE FOR SPECTRAL STATE TRANSITIONS , 2011, 1108.4405.

[28]  H. Falcke,et al.  A Radio Monitoring Survey of Ultra-Luminous X-Ray Sources , 2005, astro-ph/0502265.

[29]  M. B. Davies,et al.  Ultraluminous X-Ray Sources in External Galaxies , 2001 .

[30]  M. Servillat,et al.  THE COOL ACCRETION DISK IN ESO 243-49 HLX-1: FURTHER EVIDENCE OF AN INTERMEDIATE-MASS BLACK HOLE , 2011, 1104.2614.

[31]  R. Rosenfeld Nature , 2009, Otolaryngology--head and neck surgery : official journal of American Academy of Otolaryngology-Head and Neck Surgery.

[32]  Mitchell C. Begelman,et al.  Super-Eddington Fluxes from Thin Accretion Disks? , 2002, astro-ph/0203030.