Abstract

Understanding the mechanisms of accretion-ejection during X-ray binary (XrB) outbursts has been a problem for several decades. For instance, it is still not clear what controls the spectral evolution of these objects from the hard to the soft states and then back to the hard states at the end of the outburst, tracing the well-known hysteresis cycle in the hardness-intensity diagram. Moreover, the link between the spectral states and the presence or absence of radio emission is still highly debated. In a series of papers we developed a model composed of a truncated outer standard accretion disk (SAD, from the solution of Shakura and Sunyaev) and an inner jet emitting disk (JED). In this paradigm, the JED plays the role of the hot corona while simultaneously explaining the presence of a radio jet. Our goal is to apply for the first time direct fitting procedures of the JED-SAD model to the hard states of four outbursts of GX 339-4 observed during the 2000–2010 decade by RXTE, combined with simultaneous or quasi simultaneous ATCA observations. We built JED-SAD model tables usable in XSPEC, as well as a reflection model table based on the XILLVER model of XSPEC. We applied our model to the 452 hard state observations obtained with RXTE/PCA. We were able to correctly fit the X-ray spectra and simultaneously reproduce the radio flux with an accuracy better than 15%. We show that the functional dependency of the radio emission on the model parameters (mainly the accretion rate and the transition radius between the JED and the SAD) is similar for all the rising phases of the different outbursts of GX 339-4, but it is significantly different from the functional dependency obtained in the decaying phases. This result strongly suggests a change in the radiative and/or dynamical properties of the ejection between the beginning and the end of the outburst. We discuss possible scenarios that could explain these differences.

Highlights

  • X-ray binaries (XrBs) are formidable laboratories for the study of the accretion-ejection processes around compact objects

  • The X-ray emission is commonly believed to be produced by the inner regions of the accretion flow, whereas the radio emission is thought to originate from relativistic jets

  • The variability of the source is consistent with a very compact region (De Marco et al 2017), but the exact geometry is still a matter of debate. It could be located somewhere above the black hole. It can partly cover the accretion disk or it can fill the inner part of the accretion flow, the accretion disk being present in the outer part of the

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Summary

Introduction

X-ray binaries (XrBs) are formidable laboratories for the study of the accretion-ejection processes around compact objects. The variability of the source is consistent with a very compact region (De Marco et al 2017), but the exact geometry is still a matter of debate It could be located somewhere above the black hole (the so-called lamppost geometry, e.g., Matt et al 1991; Martocchia & Matt 1996; Miniutti & Fabian 2004). It can partly cover the accretion disk (the patchy corona geometry, e.g., Haardt et al 1997) or it can fill the inner part of the accretion flow, the accretion disk being present in the outer part of the

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