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  • A Broadband View on Microqu...
    Rodi, J.; Tramacere, A.; Onori, F.; Bruni, G.; Sànchez-Fernàndez, C.; Fiocchi, M.; Natalucci, L.; Ubertini, P.

    The Astrophysical journal, 03/2021, Letnik: 910, Številka: 1
    Journal Article

    Abstract The microquasar MAXI J1820+070 went into outburst from 2018 mid-March until mid-July, with several faint rebrightenings afterward. With a peak flux of approximately 4 Crab in the 20–50 keV energy range, the source was monitored across the electromagnetic spectrum with detections from radio to hard X-ray frequencies. Using these multiwavelength observations, we analyzed quasi-simultaneous observations from April 12, near the peak of the outburst (∼March 23). Analysis of the X-ray spectrum found it indicative of an accreting black hole binary in the hard state, consistent with the flat/inverted radio spectrum and the accretion disk winds seen at optical wavelengths. Then, we constructed a spectral energy distribution spanning ∼12 orders of magnitude using modeling in JetSeT . The model is composed of an irradiated disk with a Compton hump and a leptonic jet with an acceleration region and a synchrotron-dominated cooling region. JetSeT finds that the spectrum is dominated by jet emission up to approximately 10 14 Hz, after which disk and coronal emission dominates. The acceleration region has a magnetic field of B ∼ 1.6 × 10 4 G, a cross section of R ∼ 2.8 × 10 9 cm, and a flat radio spectral shape naturally obtained from the synchroton cooling of the accelerated electrons. The jet luminosity is >8 × 10 37 erg s −1 (>0.15 L Edd ), compared to an accretion luminosity of ∼6 × 10 37 erg s −1 , assuming a distance of 3 kpc. Because these two values are comparable, it is possible that the jet is powered predominately via accretion with only a small contribution needed from the Blanford–Znajek mechanism from the reportedly slowly spinning black hole.