Chandra X-ray spectroscopic imaging of Sagittarius A* and the central parsec of the Galaxy

We report the results of the first-epoch observation with the ACIS-I instrument on the Chandra X-Ray Observatory of Sagittarius A* (Sgr A*), the compact radio source associated with the supermassive black hole (SMBH) at the dynamical center of the Milky Way. This observation produced the first X-ray (0.5-7 keV) spectroscopic image with arcsecond resolution of the central 17' x 17' (40 pc x 40 pc) of the Galaxy. We report the discovery of an X-ray source, CXOGC J174540.0 - 290027, coincident with Sgr A* within 0.27 +/- 0.18. The probability of a false match is estimated to be less than or similar to 0.5%. The spectrum is well fitted either by an absorbed power law with photon index Gamma approximate to 2.7 or by an absorbed optically thin thermal plasma with kT approximate to 1.9 keV and column density N-H approximate to 1 x 10(23) cm(-2). The observed flux in the 2 - 10 keV band is approximate to 1.3 x 10(-13) ergs cm(-2) s(-1), and the absorption-corrected luminosity is approximate to2.4 x 10(33) ergs s(-1). The X-ray emission at the position of Sgr A* is extended, with an intrinsic size of approximate to1.4 (FWHM), consistent with the Bondi accretion radius for a 2.6 x 10(6) M. black hole. A compact component within the source flared by up to a factor of 3 over a period of approximate to1 hr at the start of the observation. The search for Kalpha line emission from iron was inconclusive, yielding an upper limit on the equivalent width of 2.2 keV. Several potential stellar origins for the X-ray emission at Sgr A* are considered, but we conclude that the various properties of the source favor accretion onto the SMBH as the origin for the bulk of the emission. These data are inconsistent with standard'' advection-dominated accretion flow (ADAF) models or Bondi models, unless the accretion rate from stellar winds is much lower than anticipated. The central parsec of the Galaxy contains an approximate to1.3 keV plasma with electron density n(e) approximate to 26(etaf)(1/2) cm(-3), where eta(f) is the filling factor. This plasma should supply approximate to 10(-6) M. yr(-1) of material to the accretion flow at the Bondi radius, whereas measurements of linear polarization at 150 GHz and above limit the accretion rate near the event horizon to less than or similar to 10(-8) M. yr(-1), assuming an equipartition magnetic field. Taken together, the X-ray and radio results imply that outflows or convection are playing a role in ADAF models and subequipartition magnetic fields in Bondi models, or else the X-ray emission must be generated predominantly via the synchrotron self-Compton (SSC) process. The measured extent of the source and the detection of short timescale variability are evidence that the emission from Sgr A* contains both thermal and nonthermal emission components at comparable levels. We also discuss the complex structure of the X-ray emission from the Sgr A radio complex and along the Galactic plane. Morphological evidence is presented that Sgr A* and the H II region Sgr A West lie within the hot plasma in the central cavity of Sgr A East, which we interpret as a supernova remnant that may have passed through the position of the SMBH, leading to a period of increased activity that ended within the past approximate to300 yr. Similarly, we have discovered bright clumps of X-ray emission located on opposite sides of the Galactic plane, along a line passing through the central parsec of the Galaxy. The arrangement of these lobes suggests that Sgr A* may have experienced an earlier period of increased activity lasting several thousand years during which it expelled hot gas in a bipolar outflow oriented roughly perpendicular to the Galactic plane. Additionally, we present an analysis of stellar emission within the central parsec of the Galaxy.