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A Thermal Bremsstrahlung Model for the Quiescent X‐Ray Emission from Sagittarius A*
Author(s) -
Eliot Quataert
Publication year - 2002
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/341425
Subject(s) - physics , astrophysics , bremsstrahlung , accretion (finance) , galactic center , active galactic nucleus , black hole (networking) , flux (metallurgy) , astronomy , radius , galaxy , electron , nuclear physics , computer network , routing protocol , routing (electronic design automation) , materials science , computer security , computer science , metallurgy , link state routing protocol
I consider the thermal bremsstrahlung emission from hot accretion flows(Bondi/ADAFs), taking into account the finite size of the observing telescope'sbeam (R_beam) relative to the Bondi accretion radius (R_A). For R_beam >> R_Asoft X-ray emission from the hot interstellar medium surrounding the black holedominates the observed emission while for R_beam << R_A hard X-ray emissionfrom the accretion flow dominates. I apply these models to Chandra observationsof the Galactic Center, for which R_beam ~ R_A. I argue that bremsstrahlungemission accounts for most of the ``quiescent'' (non-flaring) flux observed byChandra from Sgr A*; this emission is spatially extended on scales ~ R_A ~ 1''and has a relatively soft spectrum, as is observed. If accretion onto thecentral black hole proceeds via a Bondi or ADAF flow, a hard X-ray power lawshould be present in deeper observations with a flux ~ 1/3 of the soft X-rayflux; nondetection of this hard X-ray component would argue against ADAF/Bondimodels. I briefly discuss the application of these results to otherlow-luminosity AGN.Comment: final version accepted by ApJ; some rewriting but conclusions unchange

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