Disk-dominated States of 4U 1957+11: Chandra, XMM-Newton, and RXTE Observations of Ostensibly the Most Rapidly Spinning Galactic Black Hole

We present simultaneous Chandra High-Energy Transmission Gratings (HETG) and Rossi X-ray Timing Explorer (RXTE) observations of a “soft state” of the black hole candidate 4U 1957+11. These spectra, having limited hard X-ray excess, are an excellent test of disk atmosphere models that include effects of black hole spin. The HETG data show, by modeling the broadband continuum and direct fitting of absorption edges, that the disk spectrum is only very mildly absorbed, with NH = (1–2) × 1021 cm−2. These data additionally reveal λλ13.449 Ne IX absorption consistent with the warm/hot phase of the interstellar medium. The fitted disk model implies an inclined disk around a low-mass black hole rotating with normalized spin a* ≈ 1. We show, however, that pure Schwarzschild models describe the data extremely well, albeit with large disk atmosphere ``color-correction'' factors. Standard correction factors can be attained if one incorporates mild Comptonization. We find that the Chandra observations do not uniquely determine spin, even with this otherwise extremely well-measured, nearly pure disk spectrum. XMM-Newton RXTE observations, taken only six weeks later, are equally unconstraining. This lack of constraint is partly driven by the unknown mass and distance of 4U 1957+11; however, it is also driven by the limited Chandra and XMM-Newton bandpasses. We therefore present a series of 48 RXTE observations taken at different brightness/hardness levels. These data prefer a spin of a* ≈ 1, even when including a mild Comptonization component; however, they also show evolution of the color-correction factors. If the rapid-spin models with standard correction factors are to be believed, then the RXTE observations predict that 4U 1957+11 can range from a 3 M☉ black hole at 10 kpc with a* ≈ 0.83 to a 16 M☉ black hole at 22 kpc with a* ≈ 1.

[1]  C. Done,et al.  Angular Momentum Transport in Accretion Disks and Its Implications for Spin Estimates in Black Hole Binaries , 2008, 0803.0584.

[2]  U. Cambridge,et al.  The Accretion Disk Wind in the Black Hole GRO J1655–40 , 2008, 0802.2026.

[3]  N. Schulz,et al.  Limits on Hot Galactic Halo Gas from X-Ray Absorption Lines , 2007, 0711.3212.

[4]  H. Marshall,et al.  High-Resolution X-Ray Spectroscopy of a Low-Luminosity Active Galactic Nucleus: The Structure and Dynamics of M81* , 2007 .

[5]  Q. Wang,et al.  The Galactic Central Diffuse X-Ray Enhancement: A Differential Absorption/Emission Analysis , 2007, 0705.2772.

[6]  J. McClintock,et al.  X-Ray Properties of Black-Hole Binaries , 2006, astro-ph/0606352.

[7]  R. Shafee,et al.  The Spin of the Near-Extreme Kerr Black Hole GRS 1915+105 , 2006, astro-ph/0606076.

[8]  S. Sazonov,et al.  Map of the galaxy in the 6.7-keV emission line , 2006, astro-ph/0605693.

[9]  Norbert S. Schulz,et al.  High-Resolution X-Ray Spectroscopy of the Interstellar Medium. II. Neon and Iron Absorption Edges , 2006, astro-ph/0605674.

[10]  D. Steeghs,et al.  The magnetic nature of disk accretion onto black holes , 2006, Nature.

[11]  O. Blaes,et al.  Testing Accretion Disk Theory in Black Hole X-Ray Binaries , 2006, astro-ph/0602245.

[12]  M. Gierliński,et al.  Black hole spin in GRS 1915+105 , 2006, astro-ph/0601540.

[13]  R. Shafee,et al.  Estimating the Spin of Stellar-Mass Black Holes by Spectral Fitting of the X-Ray Continuum , 2005, astro-ph/0508302.

[14]  Mark L. Schattenburg,et al.  The Chandra High‐Energy Transmission Grating: Design, Fabrication, Ground Calibration, and 5 Years in Flight , 2005, astro-ph/0507035.

[15]  S. Corbel,et al.  Is the “IR Coincidence” Just That? , 2005, astro-ph/0503334.

[16]  O. Blaes,et al.  Relativistic Accretion Disk Models of High-State Black Hole X-Ray Binary Spectra , 2004, astro-ph/0408590.

[17]  R. Narayan,et al.  Multitemperature Blackbody Spectrum of a Thin Accretion Disk around a Kerr Black Hole: Model Computations and Comparison with Observations , 2004, astro-ph/0411583.

[18]  N. Schulz,et al.  High-Resolution X-Ray Spectroscopy of the Interstellar Medium: Structure at the Oxygen Absorption Edge , 2003, astro-ph/0312205.

[19]  U. Diego,et al.  Chandra/High Energy Transmission Grating Spectrometer Spectroscopy of the Galactic Black Hole GX 339–4: A Relativistic Iron Emission Line and Evidence for a Seyfert-like Warm Absorber , 2003, astro-ph/0307394.

[20]  Thomas J. Maccarone,et al.  Do X-ray binary spectral state transition luminosities vary? , 2003, astro-ph/0308036.

[21]  John E. Davis Pile-up model for dispersed spectra , 2003, SPIE Astronomical Telescopes + Instrumentation.

[22]  J. Herder,et al.  The Reflection Grating Spectrometer on-board XMM-Newton: Status of the Calibrations , 2002 .

[23]  John E. Davis,et al.  Event Pileup in Charge-coupled Devices , 2001 .

[24]  R. Wijnands,et al.  4U 1957+11: a persistent low-mass X-ray binary and black hole candidate in the high state? , 2001, astro-ph/0104395.

[25]  Los Alamos National Lab,et al.  The XMM-Newton optical/UV monitor telescope , 2000, astro-ph/0011216.

[26]  Ucsd,et al.  A good long look at the black hole candidates LMC X-1 and LMC X-3 , 2000, astro-ph/0005487.

[27]  Elmar Pfeffermann,et al.  The European Photon Imaging Camera on XMM-Newton: The pn-CCD camera , 2001 .

[28]  R. McCray,et al.  Astrophysical Journal, in press Preprint typeset using L ATEX style emulateapj v. 26/01/00 ON THE ABSORPTION OF X-RAYS IN THE INTERSTELLAR MEDIUM , 2000 .

[29]  Boulder,et al.  Soft-to-Hard State Transitions in LMC X-3 , 2000, astro-ph/0005489.

[30]  R. Wijnands,et al.  Correlated X-Ray Spectral and Timing Behavior of the Black Hole Candidate XTE J1550–564: A New Interpretation of Black Hole States , 2000, astro-ph/0001163.

[31]  J. Orosz,et al.  Correlations between Low-Frequency Quasi-periodic Oscillations and Spectral Parameters in XTE J1550–564 and GRO J1655–40 , 1999, astro-ph/9910519.

[32]  M. Nowak,et al.  On the Enigmatic X-Ray Source V1408 Aquilae (=4U 1957+11) , 1999, astro-ph/9903276.

[33]  P. Hakala,et al.  Evidence for evolving accretion disk structure in 4U 1957+115 , 1998, astro-ph/9811305.

[34]  M. Begelman,et al.  Self-consistent Thermal Accretion Disk Corona Models for Compact Objects. I. Properties of the Corona and the Spectrum of Escaping Radiation , 1997, The Astrophysical Journal.

[35]  J. E. Pringle,et al.  Self-induced warping of accretion discs , 1996 .

[36]  Lev Titarchuk,et al.  GENERALIZED COMPTONIZATION MODELS AND APPLICATION TO THE RECENT HIGH-ENERGY OBSERVATIONS , 1994 .

[37]  R. Petre,et al.  A BBXRT observation of the high-luminosity quasar H1821+643 , 1993 .

[38]  S. Kitamoto,et al.  Another Canonical Time Variation of X-Rays from Black Hole Candidates in the Very High Flare State? , 1993 .

[39]  Kazuhiro Kimura,et al.  X-ray variability of GX 339 - 4 in its very high state , 1991 .

[40]  J. Thorstensen A 9.3 hour orbital period in the potential black hole binary 4U 1957 + 11 , 1987 .