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dc.contributor.authorBassi, T.
dc.contributor.authorMalzac, J.
dc.contributor.authorDel Santo, M.
dc.contributor.authorJourdain, E.
dc.contributor.authorRoques, J.P.
dc.contributor.authorD'Aì, A.
dc.contributor.authorMiller-Jones, James
dc.contributor.authorBelmont, R.
dc.contributor.authorMotta, S.E.
dc.contributor.authorSegreto, A.
dc.contributor.authorTesta, V.
dc.contributor.authorCasella, P.
dc.date.accessioned2023-04-18T14:57:09Z
dc.date.available2023-04-18T14:57:09Z
dc.date.issued2020
dc.identifier.citationBassi, T. and Malzac, J. and Del Santo, M. and Jourdain, E. and Roques, J.P. and D'Aì, A. and Miller-Jones, J.C.A. et al. 2020. On the nature of the soft γ-ray emission in the hard state of the black hole transient GRS 1716−249. Monthly Notices of the Royal Astronomical Society. 494 (1): pp. 571-583.
dc.identifier.urihttp://hdl.handle.net/20.500.11937/91531
dc.identifier.doi10.1093/mnras/staa739
dc.description.abstract

The black hole transient GRS 1716−249 was monitored from the radio to the γ -ray band during its 2016-2017 outburst. This paper focuses on the spectral energy distribution (SED) obtained in 2017 February-March, when GRS 1716−249 was in a bright hard spectral state. The soft γ -ray data collected with the INTEGRAL/SPI telescope show the presence of a spectral component that is in excess of the thermal Comptonization emission. This component is usually interpreted as inverse Compton emission from a tiny fraction of non-thermal electrons in the X-ray corona. We find that hybrid thermal/non-thermal Comptonization models provide a good fit to the X-/γ -ray spectrum of GRS 1716−249. The best-fitting parameters are typical of the bright hard state spectra observed in other black hole X-ray binaries. Moreover, the magnetized hybrid Comptonization model BELM provides an upper limit on the intensity of the coronal magnetic field of about 106 G. Alternatively, this soft γ -ray emission could originate from synchrotron emission in the radio jet. In order to test this hypothesis, we fit the SED with the irradiated disc plus Comptonization model combined with the jet internal shock emission model ISHEM. We found that a jet with an electron distribution of p = 2.1 can reproduce the soft γ -ray emission of GRS 1716−249. However, if we introduce the expected cooling break around 10 keV, the jet model can no longer explain the observed soft γ -ray emission, unless the index of the electron energy distribution is significantly harder (p < 2).

dc.languageEnglish
dc.publisherOXFORD UNIV PRESS
dc.relation.sponsoredbyhttp://purl.org/au-research/grants/arc/FT140101082
dc.subjectScience & Technology
dc.subjectPhysical Sciences
dc.subjectAstronomy & Astrophysics
dc.subjectaccretion, accretion discs
dc.subjectblack hole physics
dc.subjectISM: jets and outflows
dc.subjectgammarays: general
dc.subjectX-rays: binaries
dc.subjectSPECTRAL ENERGY-DISTRIBUTION
dc.subjectX-RAY
dc.subjectCOMPACT JET
dc.subjectINTERNAL SHOCKS
dc.subjectCYGNUS X-1
dc.subjectACCRETION
dc.subjectRADIO
dc.subjectVARIABILITY
dc.subjectSYNCHROTRON
dc.subjectRADIATION
dc.titleOn the nature of the soft γ-ray emission in the hard state of the black hole transient GRS 1716−249
dc.typeJournal Article
dcterms.source.volume494
dcterms.source.number1
dcterms.source.startPage571
dcterms.source.endPage583
dcterms.source.issn0035-8711
dcterms.source.titleMonthly Notices of the Royal Astronomical Society
dc.date.updated2023-04-18T14:57:08Z
curtin.departmentSchool of Elec Eng, Comp and Math Sci (EECMS)
curtin.accessStatusOpen access
curtin.facultyFaculty of Science and Engineering
curtin.contributor.orcidMiller-Jones, James [0000-0003-3124-2814]
curtin.contributor.researcheridMiller-Jones, James [B-2411-2013]
curtin.locationThis article has been accepted for publication in Monthly Notices of the Royal Astronomical Society ©: 2020 The Author(s). Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.
dcterms.source.eissn1365-2966
curtin.contributor.scopusauthoridMiller-Jones, James [10044231400]
curtin.repositoryagreementV3


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