Journal
ASTROPHYSICAL JOURNAL
Volume 755, Issue 2, Pages -Publisher
IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/755/2/133
Keywords
accretion, accretion disks; black hole physics; Galaxy: center; polarization; radiative transfer; relativistic processes
Categories
Funding
- NSF [TG-AST080025N, TG-AST080026N]
- NASA [NNX08AX04H, NNX08AH32G, NNX11AE16G, HST-HF-51298.01, PF7-80048]
- NASA [93749, NNX08AX04H] Funding Source: Federal RePORTER
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We obtain estimates of Sgr A* accretion flow and black hole parameters by fitting polarized submillimeter observations with spectra computed using three-dimensional general relativistic (GR) magnetohydrodynamical (MHD) (GRMHD) simulations. Observations are compiled from averages over many epochs from reports in 29 papers for estimating the mean fluxes F-nu, linear polarization (LP) fractions, circular polarization (CP) fractions, and electric vector position angles. GRMHD simulations are computed with dimensionless spins a(*) = 0, 0.5, 0.7, 0.9, 0.98 over a 20,000 M time interval. We perform fully self-consistent GR polarized radiative transfer using our new code to explore the effects of spin a*, inclination angle theta, position angle (P. A.), accretion rate (M) over dot, and electron temperature T-e (T-e is reported for radius 6M). By fitting the mean submillimeter fluxes and LP/CP fractions, we obtain estimates for these model parameters and determine the physical effects that could produce polarization signatures. Our best-bet model has a(*) = 0.5, theta = 75 degrees, P.A. = 115 degrees, (M) over dot = 4.6 x 10(-8) M-circle dot yr(-1), and T-e = 3.1x10(10) K at 6M. The submillimeter CP is mainly produced by Faraday conversion as modified by Faraday rotation, and the emission region size at 230 GHz is consistent with the very long baseline interferometry size of 37 mu as. Across all spins, model parameters are in the ranges theta = 42 degrees-75 degrees, (M) over dot = (1.4-7.0) x 10(-8) M-circle dot yr(-1), and T-e = (3-4) x 10(10) K. Polarization is found both to help differentiate models and to introduce new observational constraints on the effects of the magnetic field that might not be fit by accretion models so far considered.
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