Publications (3)0 Total impact
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ABSTRACT: Ongoing millimeter VLBI observations with the Event Horizon Telescope allow
unprecedented study of the innermost portion of black hole accretion flows.
Interpreting the observations requires relativistic, time-dependent physical
modeling. We discuss the comparison of radiative transfer calculations from
general relativistic MHD simulations of Sagittarius A* and M87 with current and
future mm-VLBI observations. This comparison allows estimates of the viewing
geometry and physical conditions of the Sgr A* accretion flow. The viewing
geometry for M87 is already constrained from observations of its large-scale
jet, but, unlike Sgr A*, there is no consensus for its millimeter emission
geometry or electron population. Despite this uncertainty, as long as the
emission region is compact, robust predictions for the size of its jet
launching region can be made. For both sources, the black hole shadow may be
detected with future observations including ALMA and/or the LMT, which would
constitute the first direct evidence for a black hole event horizon.
02/2012;
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ABSTRACT: The supermassive black hole candidate at the center of M87 drives an
ultra-relativistic jet visible on kiloparsec scales, and its large mass and
relative proximity allow for event horizon scale imaging with very long
baseline interferometry at millimeter wavelengths (mm-VLBI). Recently,
relativistic magneto-hydrodynamic (MHD) simulations of black hole accretion
flows have proven capable of launching magnetically-dominated jets. We
construct time-dependent disc/jet models of the innermost portion of the M87
nucleus by performing relativistic radiative transfer calculations from one
such simulation. We identify two types of models, jet-dominated or disc/jet,
that can explain the spectral properties of M87, and use them to make
predictions for current and future mm-VLBI observations. The Gaussian source
size for the favored sky orientation and inclination from observations of the
large-scale jet is 33-44 microarcseconds (~4-6 Schwarzschild radii) on current
mm-VLBI telescopes, very similar to existing observations of Sgr A*. The black
hole shadow, direct evidence of an event horizon, should be visible in future
measurements using baselines between Hawaii and Mexico. Both models exhibit
variability at millimeter wavelengths with factor of ~2 amplitudes on year
timescales. For the low inclination of M87, the counter-jet dominates the event
horizon scale millimeter wavelength emission from the jet-forming region.
09/2011;
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ABSTRACT: Recent high resolution observations of the Galactic center black hole allow for direct comparison with accretion disk simulations. We compare two-temperature synchrotron emission models from three dimensional, general relativistic magnetohydrodynamic simulations to millimeter observations of Sgr A*. Fits to very long baseline interferometry and spectral index measurements disfavor the monochromatic face-on black hole shadow models from our previous work. Inclination angles \le 20 degrees are ruled out to 3 \sigma. We estimate the inclination and position angles of the black hole, as well as the electron temperature of the accretion flow and the accretion rate, to be i=50+35-15 degrees, \xi=-23+97-22 degrees, T_e=(5.4 +/- 3.0)x10^10 K and Mdot=(5+15-2)x10^-9 M_sun / yr respectively, with 90% confidence. The black hole shadow is unobscured in all best fit models, and may be detected by observations on baselines between Chile and California, Arizona or Mexico at 1.3mm or .87mm either through direct sampling of the visibility amplitude or using closure phase information. Millimeter flaring behavior consistent with the observations is present in all viable models, and is caused by magnetic turbulence in the inner radii of the accretion flow. The variability at optically thin frequencies is strongly correlated with that in the accretion rate. The simulations provide a universal picture of the 1.3mm emission region as a small region near the midplane in the inner radii of the accretion flow, which is roughly isothermal and has \nu/\nu_c ~ 1-20, where \nu_c is the critical frequency for thermal synchrotron emission. Comment: 14 pages, 17 figures, accepted by ApJ
05/2010;
Institutions
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2010–2012
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Stanford University
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Kavli Institute for Particle Physics and Cosmology (KIPAC)
Palo Alto,
CA,
USA