Intrinsic Size of Sagittarius A*: 72 Schwarzschild Radii

Recent proper motion studies of stars at the very center of the Galaxy strongly suggest that Sagittarius A*, the compact nonthermal radio source at the Galactic center, is a 2.5×106 M☉ black hole. By means of near-simultaneous multiwavelength Very Long Baseline Array measurements, we determine for the first time the intrinsic size and shape of Sgr A* to be 72 Rsc(⋆) by less than 20 Rsc(⋆), with the major axis oriented essentially north-south, where Rsc(⋆) (≡ 7.5×1011 cm) is the Schwarzschild radius for a 2.5×106 M☉ black hole. Contrary to previous expectation that the intrinsic structure of Sgr A* is observable only at λ≤1 mm, we can discern the intrinsic source size at λ=7 mm because (1) the scattering size along the minor axis is half that along the major axis and (2) the near-simultaneous multiwavelength mapping of Sgr A* with the same interferometer makes it possible to extrapolate precisely the minor axis scattering angle at λ=7 mm. The intrinsic size and shape place direct constraints on the various emission models for Sgr A*. In particular, the advection-dominated accretion flow model may have to incorporate a radio jet in order to account for the structure of Sgr A*.

[1]  G. Bower,et al.  7 Millimeter VLBA Observations of Sagittarius A* , 1998, astro-ph/9802030.

[2]  H. Falcke,et al.  The Simultaneous Spectrum of Sagittarius A* from 20 Centimeters to 1 Millimeter and the Nature of the Millimeter Excess , 1998, astro-ph/9801085.

[3]  J. Carlstrom,et al.  High-Frequency Measurements of the Spectrum of Sagittarius A* , 1997 .

[4]  Jonathan E. Grindlay,et al.  Advection-dominated Accretion Model of Sagittarius A*: Evidence for a Black Hole at the Galactic Center , 1997, astro-ph/9706112.

[5]  Reinhard Genzel,et al.  Stellar proper motions in the central 0.1 PC of the galaxy , 1997 .

[6]  A. Eckart,et al.  Observations of stellar proper motions near the Galactic Centre , 1996, Nature.

[7]  S. Padin,et al.  Small-scale structure and position of Sagittarius A(*) from VLBI at 3 millimeter wavelength , 1994 .

[8]  S. Sridhar,et al.  Toward a theory of interstellar turbulence. 2. Strong Alfvenic turbulence , 1994 .

[9]  Fulvio Melia,et al.  An accreting black hole model for Sagittarius A(*). 2: A detailed study , 1994 .

[10]  J. Moran,et al.  Upper Limit of 3.3 Astronomical Units to the Diameter of the Galactic Center Radio Source Sgr A* , 1993, Science.

[11]  W. Goss,et al.  High-resolution VLBA imaging of the radio source Sgr A* at the Galactic Centre , 1993, Nature.

[12]  F. Melia,et al.  A determination of the mass of Sagittarius A* from its radio spectral and source size measurements , 1992 .

[13]  C. Gwinn,et al.  The Galactic center radio source shines below the Compton limit , 1991 .

[14]  W. Hubbard,et al.  Theory of anisotropic refractive scintillation - Application to stellar occultations by Neptune , 1988 .

[15]  R. Blandford,et al.  Refractive effects in pulsar scintillation , 1986 .

[16]  J. M. Moran,et al.  On the size of the galactic centre compact radio source: diameter <20 AU , 1985, Nature.

[17]  J. Higdon Density fluctuations in the interstellar medium: evidence for anisotropic magnetogasdynamic turbulen , 1984 .

[18]  M. Cohen,et al.  Multiwavelength VLBI observations of the galactic center , 1981 .

[19]  S. Reynolds,et al.  Synchrotron Radiation from Relativistic Winds, with an Application to the Compact Radio Source at the Galactic Center , 1980 .

[20]  D. Walsh,et al.  The Radio Source at the Galactic Nucleus , 1976 .

[21]  R. L. Brown,et al.  Intense sub-arcsecond structure in the galactic center , 1974 .

[22]  M. Rees,et al.  On Quasars, Dust and the Galactic Centre , 1971 .