Regulation of Black Hole Winds and Jets across the Mass Scale

Authors

A. L. King, University of Michigan
J. M. Miller, University of Michigan
J. Raymond, Smithsonian Astrophysical Observatory
A. C. Fabian, Institute of Astronomy, University of Cambridge
C. S. Reynolds, University of Maryland
K. Gültekin, University of Michigan
E. M. Cackett, Institute of Astronomy, University of CambridgeFollow
S. W. Allen, Kavli Institute for Particle Astrophysics and Cosmology, Stanford University
D. Proga, University of Nevada
T. R. Kallman, Laboratory for High Energy Astrophysics, NASA Goddard Space Flight Center

Document Type

Article

Abstract

We present a study of the mechanical power generated by both winds and jets across the black hole mass scale. We begin with the study of ionized X-ray winds and present a uniform analysis using Chandra grating spectra. The high-quality grating spectra facilitate the characterization of the outflow velocity, ionization, and column density of the absorbing gas. We find that the kinetic power of the winds, derived from these observed quantities, scales with increasing bolometric luminosity as log (L _{wind, 42}/C_v ) = (1.58 ± 0.07)log (L _{Bol, 42}) - (3.19 ± 0.19). This suggests that supermassive black holes may be more efficient than stellar-mass black holes in launching winds, per unit filling factor, C_v . If the black hole binary (BHB) and active galactic nucleus (AGN) samples are fit individually, the slopes flatten to α^BHB = 0.91 ± 0.31 and α^AGN = 0.63 ± 0.30 (formally consistent within errors). The broad fit and individual fits both characterize the data fairly well, and the possibility of common slopes may point to common driving mechanisms across the mass scale. For comparison, we examine jet production, estimating jet power based on the energy required to inflate local bubbles. The jet relation is log (L _{Jet, 42}) = (1.18 ± 0.24)log (L _{Bondi, 42}) - (0.96 ± 0.43). The energetics of the bubble associated with Cygnus X-1 are particularly difficult to determine, and the bubble could be a background supernova remnant. If we exclude Cygnus X-1 from our fits, then the jets follow a relation consistent with the winds, but with a higher intercept, log (L _{Jet, 42}) = (1.34 ± 0.50)log (L _{Bondi, 42}) - (0.80 ± 0.82). The formal consistency in the wind and jet scaling relations, when assuming that L _Bol and L _Bondi are both proxies for mass accretion rate, suggests that a common launching mechanism may drive both flows; magnetic processes, such as magnetohydrodynamics and magnetocentrifugal forces, are viable possibilities. We also examine winds that are moving at especially high velocities, v > 0.01c. These ultra-fast outflows tend to resemble the jets more than the winds in terms of outflow power, indicating that we may be observing a regime in which winds become jets. A transition at approximately L _Bol ≈ 10^-2 L _Edd is apparent when outflow power is plotted versus Eddington fraction. At low Eddington fractions, the jet power is dominant, and at high Eddington fractions, the wind power is dominant. This study allows for the total power from black hole accretion, both mechanical and radiative, to be characterized in a simple manner and suggests possible connections between winds and jets. X-ray wind data and jet cavity data will enable stronger tests.

Disciplines

Cosmology, Relativity, and Gravity | External Galaxies

Comments

NOTICE IN COMPLIANCE WITH PUBLISHER POLICY: ©2013, American Astronomical Society. Available at: doi:10.1088/0004-637X/762/2/103

Recommended Citation

Regulation of Black Hole Winds and Jets across the Mass Scale

A. L. King et al. 2013 ApJ 762 103