Constraining the Structure of Sagittarius A*'s Accretion Flow with Millimeter Very Long Baseline Interferometry Closure Phases

Citation:

Avery E. Broderick, Vincent L. Fish, Sheperd S. Doeleman, and Abraham Loeb. 2011. “Constraining the Structure of Sagittarius A*'s Accretion Flow with Millimeter Very Long Baseline Interferometry Closure Phases.” The Astrophysical Journal, 738.

Abstract:

Millimeter wave very long baseline interferometry (mm-VLBI) providesaccess to the emission region surrounding Sagittarius A* (Sgr A*), thesupermassive black hole at the center of the Milky Way, on sub-horizonscales. Recently, a closure phase of 0° ± 40° wasreported on a triangle of Earth-sized baselines (SMT-CARMA-JCMT)representing a new constraint upon the structure and orientation of theemission region, independent from those provided by the previouslymeasured 1.3 mm-VLBI visibility amplitudes alone. Here, we compare thisto the closure phases associated with a class of physically motivated,radiatively inefficient accretion flow models and present predictionsfor future mm-VLBI experiments with the developing Event HorizonTelescope (EHT). We find that the accretion flow models are capable ofproducing a wide variety of closure phases on the SMT-CARMA-JCMTtriangle and thus not all models are consistent with the recentobservations. However, those models that reproduce the 1.3 mm-VLBIvisibility amplitudes overwhelmingly have SMT-CARMA-JCMT closure phasesbetween ±30°, and are therefore broadly consistent with allcurrent mm-VLBI observations. Improving station sensitivity by factorsof a few, achievable by increases in bandwidth and phasing togethermultiple antennas at individual sites, should result in physicallyrelevant additional constraints upon the model parameters and eliminatethe current 180° ambiguity on the source orientation. Whenadditional stations are included, closure phases of order45°-90° are typical. In all cases, the EHT will be able tomeasure these with sufficient precision to produce dramatic improvementsin the constraints upon the spin of Sgr A*.