2018
DOI: 10.3847/1538-4357/aabe2e
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Detection of Intrinsic Source Structure at ∼3 Schwarzschild Radii with Millimeter-VLBI Observations of SAGITTARIUS A*

Abstract: We report results from very long baseline interferometric (VLBI) observations of the supermassive black hole in the Galactic center, Sgr A*, at 1.3 mm (230 GHz). The observations were performed in 2013 March using six VLBI stations in Hawaii, California, Arizona, and Chile. Compared to earlier observations, the addition of the APEX telescope in Chile almost doubles the longest baseline length in the array, provides additional uv coverage in the N–S direction, and leads to a spatial resolution of ∼30 μas (∼3 Sc… Show more

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Cited by 88 publications
(59 citation statements)
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“…Further, the current EHT array is missing short baseline coverage, and an orbit that never crosses the face of the Earth as seen from Sgr A* would form short baselines primarily with sites that had just come into view; these sites would be looking through the largest possible amount of atmosphere, and thus short-baseline coverage would be less sensitive than for other orbital orientations. Baselines from the ground to a single "face-on" orbiter still have thermal noise approximately equal to those between ground sites as shown in Figure 3, and significantly lower than the long-baseline flux densities of Sgr A* at 230 GHz (Lu et al 2018), suggesting that even long-baseline observations with orbiters will produce detections.…”
Section: Orbit Design and Simulationmentioning
confidence: 97%
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“…Further, the current EHT array is missing short baseline coverage, and an orbit that never crosses the face of the Earth as seen from Sgr A* would form short baselines primarily with sites that had just come into view; these sites would be looking through the largest possible amount of atmosphere, and thus short-baseline coverage would be less sensitive than for other orbital orientations. Baselines from the ground to a single "face-on" orbiter still have thermal noise approximately equal to those between ground sites as shown in Figure 3, and significantly lower than the long-baseline flux densities of Sgr A* at 230 GHz (Lu et al 2018), suggesting that even long-baseline observations with orbiters will produce detections.…”
Section: Orbit Design and Simulationmentioning
confidence: 97%
“…We choose a desired thermal noise of 10 mJy based on longbaseline (∼ 7 Gλ) correlated flux densities of tenths of Janskys observed for Sgr A* (Lu et al 2018). This approximate mean sensitivity over a full observing track yields a required τ min ≈ 1 second for space-ALMA baselines.…”
Section: Basic Requirements For Space-vlbimentioning
confidence: 99%
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“…For SgrA * , the black hole candidate at the Galactic center with a presumed mass of M 4 10 6  (Balick & Brown 1974;Ghez et al 2008;Genzel et al 2010;GRAVITY Collaboration et al 2018a), the 1.3 mm emission has been measured to have a size of 3.7 R s (Doeleman et al 2008;Fish et al 2011). More recently, full polarimetric VLBI observations at 1.3 mm wavelength have revealed ordered and time-variable magnetic fields within SgrA * on horizon scales (Johnson et al 2015), and extension to longer baselines has confirmed compact structure on ∼3 R s scales (Lu et al 2018). These results, obtained with three-and four-site VLBI arrays consisting of the former Combined Array for Research in Millimeter-wave Astronomy (CARMA) in California, the Submillimeter Telescope (SMT) in Arizona, the James Clerk Maxwell Telescope (JCMT) and Submillimeter Array (SMA) facilities on Maunakea in Hawaii, and the Atacama Pathfinder Experiment (APEX) telescope in Chile, demonstrated that direct imaging of emission structures near the event horizon of SMBH candidates is possible in principle.…”
Section: Target Sources and Confirmation Of Horizon-scale Structurementioning
confidence: 99%
“…It has long been a target of radio very long baseline interferometry (VLBI, Lo et al 1975;Backer 1978;Krichbaum et al 1998;Bower et al 2006). With 1.3mm VLBI, the source size is as compact as 8 − 10r g (Doeleman et al 2008;Fish et al 2011;Lu et al 2018;Johnson et al 2018), where r g = GM/c 2 6 × 10 11 cm is the gravitational radius.…”
Section: Introductionmentioning
confidence: 99%