Multistructured Accretion Flow of Sgr A*. I Examination of a Radiatively Inefficient Accretion Flow Model

Open Access
Authors
  • D. Haggard
  • Q.D. Wang
  • J. Neilsen
  • C.M.P. Russell
  • D. Calderón
  • J. Cuadra
  • F. Baganoff
Publication date 10-10-2024
Journal Astrophysical Journal
Article number 98
Volume | Issue number 974 | 1
Number of pages 9
Organisations
  • Faculty of Science (FNWI) - Anton Pannekoek Institute for Astronomy (API)
Abstract
The extreme low-luminosity supermassive black hole Sgr A* provides a unique laboratory in which to test models of radiatively inefficient accretion flows (RIAFs). Previous fits to the quiescent Chandra ACIS-S spectrum found that a RIAF model with an equal inflow–outflow balance works well. In this work, we apply the RIAF model to the Chandra HETG-S spectrum obtained through the Chandra X-ray Visionary Program, which displays features suggestive of temperature and velocity structures within the plasma. A comprehensive forward model analysis accounting for the accretion flow geometry and HETG-S instrumental effects is required for a full interpretation of the quiescent Chandra HETG-S spectrum. We present a RIAF model that takes these effects into account. Our fits to the high-resolution grating spectrum indicate an inflow balanced by an outflow (s ∼ 1) alongside a temperature profile that appears shallower than what would be expected from a gravitational potential following 1/r. The data require that the abundance of iron relative to solar is ZFe < 0.32 Z (90% credible interval), much lower than the 2 Z metallicity measured in nearby late-type giants. While future missions like NewAthena will provide higher spectral resolution, source separation will continue to be a problem. Leveraging Chandra's unparalleled spatial resolution, which is not expected to be surpassed for decades, remains essential for detailed investigations of the densely populated Galactic center in X-rays.
Document type Article
Language English
Published at https://doi.org/10.3847/1538-4357/ad6c08
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