2014MNRAS.441.1005D


Query : 2014MNRAS.441.1005D

2014MNRAS.441.1005D - Mon. Not. R. Astron. Soc., 441, 1005-1016 (2014/June-3)

Exploring plasma evolution during Sagittarius A* flares.

DIBI S., MARKOFF S., BELMONT R., MALZAC J., BARRIERE N.M. and TOMSICK J.A.

Abstract (from CDS):

We present a new way of describing the flares from Sgr A* with a self-consistent calculation of the particle distribution. All relevant radiative processes are taken into account in the evolution of the electron distribution and resulting spectrum. We present spectral modelling for new X-ray flares observed by NuSTAR, together with older observations in different wavelengths, and discuss the changes in plasma parameters to produce a flare. We show that under certain conditions, the real particle distribution can differ significantly from standard distributions assumed in most studies. We conclude that the flares are likely generated by magnetized plasma consistent with our understanding of the accretion flow. Including non-thermal acceleration, injection, escape, and cooling losses produces a spectrum with a break between the infrared and the X-ray, allowing a better simultaneous description of the different wavelengths. We favour the non-thermal synchrotron interpretation, assuming the infrared flare spectrum used is representative. We also consider the effects on Sgr A*'s quiescent spectrum in the case of a density increase due to the G2 encounter with Sgr A*.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): accretion, accretion discs - black hole physics - MHD - radiation mechanisms: general - Galaxy: centre

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
2 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4970 3
3 NAME G2 Dust Cloud IR 17 45 40.04 -29 00 28.1           ~ 209 0

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