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High-density reflection spectroscopy: I. A case study of GX 339-4

Jiachen JiangInstitute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UKA. C. FabianInstitute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UKJingyi WangMIT Kavli Institute for Astrophysics and Space Research, MIT, 70 Vassar Street, Cambridge, MA 02139, USAD. J. WaltonInstitute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA, UKJavier A. GarcíaCahill Center for Astronomy and Astrophysics, California Institute of Technology, Pasadena, CA 91125, USAM. L. ParkerEuropean Space Agency (ESA), European Space Astronomy Centre (ESAC), E-28691 Villanueva de la Cañada, SpainJames F. SteinerMIT Kavli Institute for Astrophysics and Space Research, MIT, 70 Vassar Street, Cambridge, MA 02139, USAJohn A. TomsickSpace Sciences Laboratory, 7 Gauss Way, University of California, Berkeley, CA 94720, USA
2019en
ABI

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We present a broad-band spectral analysis of the black hole binary GX 339-4 with NuSTAR and Swift using high-density reflection model. The observations were taken when the source was in low-flux (LF) hard states during the outbursts in 2013 and 2015, and in a very high-flux (HF) soft state in 2015. The high-density reflection model can explain its LF spectra with no requirement for an additional low temperature thermal component. This model enables us to constrain the density in the disc surface of GX 339-4 in different flux states. The disc density in the LF state is log (ne/ cm^(−3)) ≈ 21, 100 times higher than the density in the HF state (log (n_e/ cm^(−3)) = 18.93^(+0.12)_(−0.16). A close-to-solar iron abundance is obtained by modelling the LF and HF broad-band spectra with variable density reflection model (⁠Z_(Fe) = 1.50^(+0.12)_(−0.04)Z⊙ and Z_(Fe) = 1.05^(+0.17)_(−0.15)Z⊙, respectively).

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