scholarly journals ChandraX‐Ray Spectroscopic Imaging of Sagittarius A* and the Central Parsec of the Galaxy

2003 ◽  
Vol 591 (2) ◽  
pp. 891-915 ◽  
Author(s):  
F. K. Baganoff ◽  
Y. Maeda ◽  
M. Morris ◽  
M. W. Bautz ◽  
W. N. Brandt ◽  
...  
2019 ◽  
Vol 885 (2) ◽  
pp. 142 ◽  
Author(s):  
Kaya Mori ◽  
Charles J. Hailey ◽  
Shifra Mandel ◽  
Yve E. Schutt ◽  
Matteo Bachetti ◽  
...  
Keyword(s):  
X Ray ◽  

2006 ◽  
Vol 2 (14) ◽  
pp. 207-207
Author(s):  
Fabrice Martins ◽  
Reinhard Genzel ◽  
Frank Eisenhauer ◽  
Thibaut Paumard ◽  
Thomas Ott ◽  
...  

AbstractThe stellar and wind properties of the new population of massive stars in the central parsec of the Galaxy are derived through quantitative analysis with atmosphere models.


1994 ◽  
Vol 158 ◽  
pp. 379-381
Author(s):  
A. Eckart ◽  
R. Genzel ◽  
R. Hofmann ◽  
B.J. Sams ◽  
L.E. Tacconi-Garman

We present deep 1.6 and 2.2 μm images of the central parsec of the Galaxy at a resolution of 0.15″. Most of the flux in earlier seeing limited images comes from about 340 unresolved stellar sources with K≤14. The IRS 16 and 13 complexes are resolved into about two dozen and half a dozen sources, a number of which are probably luminous hot stars. We confirm the presence of a blue near infrared object (K≈13) at the position of the compact radio source Sgr A∗. The spatial centroid of the source number distribution is consistent with the position of Sgr A∗ but not with a position in the IRS 16 complex. The stellar surface density in the central 10″ is very well fitted by an isothermal cluster model with a well defined core radius. The derived core radius of all 340 sources is 0.15±0.05 pc. The central stellar density is a few times 107 M⊙ pc−3. Buildup of massive stars by merging of lower mass stars and collisional disruption of giant atmospheres are very probable processes in the central 0.2 pc.


2010 ◽  
Vol 723 (2) ◽  
pp. 1097-1109 ◽  
Author(s):  
Jun-Hui Zhao ◽  
Ray Blundell ◽  
James M. Moran ◽  
Dennis Downes ◽  
Karl F. Schuster ◽  
...  

2018 ◽  
Vol 476 (1) ◽  
pp. 235-245 ◽  
Author(s):  
P F Roche ◽  
E Lopez-Rodriguez ◽  
C M Telesco ◽  
R Schödel ◽  
C Packham

1996 ◽  
Vol 459 ◽  
pp. 627 ◽  
Author(s):  
D. A. Roberts ◽  
F. Yusef-Zadeh ◽  
W. M. Goss
Keyword(s):  

1996 ◽  
Vol 467 ◽  
pp. 645 ◽  
Author(s):  
M. Tamura ◽  
M. W. Werner ◽  
E. E. Becklin ◽  
E. S. Phinney
Keyword(s):  

2020 ◽  
Vol 644 ◽  
pp. A72
Author(s):  
J. Palouš ◽  
S. Ehlerová ◽  
R. Wünsch ◽  
M. R. Morris

Aims. We simulate shells created by supernovae expanding into the interstellar medium of the nuclear region of a galaxy, and analyze how the shell evolution is influenced by the supernova position relative to the galactic center, by the interstellar matter density, and by the combined gravitational pull of the nuclear star cluster and supermassive black hole (SMBH). Methods. We adopted simplified hydrodynamical simulations using the infinitesimally thin layer approximation in 3D (code RING) and determined whether and where the shell expansion may bring new gas into the inner parsec around the SMBH. Results. The simulations show that supernovae occurring within a conical region around the rotational axis of the galaxy can feed the central accretion disk surrounding the SMBH. For ambient densities between 103 and 105 cm−3, the average mass deposited into the central parsec by individual supernovae varies between 10 and 1000 solar masses depending on the ambient density and the spatial distribution of supernova events. Supernovae occurring in the aftermath of a starburst event near a galactic center can supply two to three orders of magnitude more mass into the central parsec, depending on the magnitude of the starburst. The deposited mass typically encounters and joins an accretion disk. The fate of that mass is then divided between the growth of the SMBH and an energetically driven outflow from the disk.


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