Modelling the compact jet in MAXI J1836-194 with disc-driven shocks

The black hole candidate MAXI J1836-194 was discovered in 2011 when it went into an outburst, and was the subject of numerous, quasi-simultaneous, multi-wavelength observations in the radio, infrared, optical, and X-rays. In this paper, we model its multi-wavelength radio to optical spectral energy...

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Published inMonthly notices of the Royal Astronomical Society Vol. 482; no. 2; pp. 2447 - 2458
Main Authors Péault, M, Malzac, J, Coriat, M, Russell, T D, Koljonen, K I I, Belmont, R, Corbel, S, Drappeau, S, Ferreira, J, Petrucci, P O, Rodriguez, J, Russell, D M
Format Journal Article
LanguageEnglish
Published Oxford University Press (OUP): Policy P - Oxford Open Option A 11.01.2019
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ISSN0035-8711
1365-2966
DOI10.1093/mnras/sty2796

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Abstract The black hole candidate MAXI J1836-194 was discovered in 2011 when it went into an outburst, and was the subject of numerous, quasi-simultaneous, multi-wavelength observations in the radio, infrared, optical, and X-rays. In this paper, we model its multi-wavelength radio to optical spectral energy distributions (SEDs) with an internal shock jet model (ishem; Malzac 2014). The jet emission is modelled on five dates of the outburst, during which the source is in the hard and hard intermediate X-ray spectral states. The model assumes that fluctuations of the jet velocity are driven by the variability in the accretion flow which is traced by the observed X-ray timing properties of the source. While the global shape of the SED is well reproduced by this model for all the studied observations, the variations in bolometric flux and typical energies require at least two parameters to evolve during the outburst. Here, we investigate variations of the jet power and mean Lorentz factor, which are both found to increase with the source luminosity. Our results are compatible with the evolution of the jet Lorentz factor reported in earlier studies of this source. However, due to the large degeneracy of the parameters of the ishem model, our proposed scenario is not unique.
AbstractList The black hole candidate MAXI J1836-194 was discovered in 2011 when it went into an outburst, and was the subject of numerous, quasi-simultaneous, multi-wavelength observations in the radio, infrared, optical, and X-rays. In this paper, we model its multi-wavelength radio to optical spectral energy distributions (SEDs) with an internal shock jet model (ishem; Malzac 2014). The jet emission is modelled on five dates of the outburst, during which the source is in the hard and hard intermediate X-ray spectral states. The model assumes that fluctuations of the jet velocity are driven by the variability in the accretion flow which is traced by the observed X-ray timing properties of the source. While the global shape of the SED is well reproduced by this model for all the studied observations, the variations in bolometric flux and typical energies require at least two parameters to evolve during the outburst. Here, we investigate variations of the jet power and mean Lorentz factor, which are both found to increase with the source luminosity. Our results are compatible with the evolution of the jet Lorentz factor reported in earlier studies of this source. However, due to the large degeneracy of the parameters of the ishem model, our proposed scenario is not unique.
Author Rodriguez, J
Koljonen, K I I
Corbel, S
Ferreira, J
Russell, T D
Coriat, M
Péault, M
Drappeau, S
Russell, D M
Malzac, J
Petrucci, P O
Belmont, R
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  organization: Université Grenoble Alpes, CNRS, IPAG, F-38000 Grenoble, France
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  organization: New York University Abu Dhabi, PO Box 129188, Abu Dhabi, UAE
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Issue 2
Keywords relativistic processes
accretion
X-rays: binaries
black hole physics
accretion discs
shock waves
Language English
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Snippet The black hole candidate MAXI J1836-194 was discovered in 2011 when it went into an outburst, and was the subject of numerous, quasi-simultaneous,...
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SubjectTerms Astrophysics
Physics
Title Modelling the compact jet in MAXI J1836-194 with disc-driven shocks
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