Volume 389, Issue 1 pp. 423-428

Origin of X-ray emission from transient black hole candidates in quiescence

Gabor Pszota

Corresponding Author

Gabor Pszota

Department of Physics, Purdue University, West Lafayette, IN 47907, USA

E-mail: [email protected] (GP); [email protected] (HZ); [email protected] (FY); [email protected] (WC)Search for more papers by this author
Hui Zhang

Corresponding Author

Hui Zhang

Shanghai Astronomical Observatory, Chinese Academy of Sciences, 200030 Shanghai, China

E-mail: [email protected] (GP); [email protected] (HZ); [email protected] (FY); [email protected] (WC)Search for more papers by this author
Feng Yuan

Corresponding Author

Feng Yuan

Shanghai Astronomical Observatory, Chinese Academy of Sciences, 200030 Shanghai, China

Joint Institute for Galaxy and Cosmology of Shanghai Astronomical Observatory, University of Science and Technology of China, China

E-mail: [email protected] (GP); [email protected] (HZ); [email protected] (FY); [email protected] (WC)Search for more papers by this author
Wei Cui

Corresponding Author

Wei Cui

Department of Physics, Purdue University, West Lafayette, IN 47907, USA

E-mail: [email protected] (GP); [email protected] (HZ); [email protected] (FY); [email protected] (WC)Search for more papers by this author
First published: 18 August 2008
Citations: 2

ABSTRACT

We report results from a systematic study of X-ray emission from black hole transients in quiescence. In this state, mass accretion is thought to follow the geometry of an outer optically thick, geometrically thin disc and an inner optically thin, geometrically thick radiatively inefficient accretion flow (RIAF). The inner flow is likely also coupled to the jets near the black hole that are often seen in such systems. The goal of the study is to see whether the X-ray emission in the quiescent state is mainly powered by the accretion flow or by the jets. Using data from deep XMMNewton observations of selected black hole transients, we have found that the quiescent X-ray spectra are, to a high precision, of power-law shape in the cases of GRO J1655-40 and V404 Cyg. Such spectra deviate significantly from the expected X-ray spectrum of the RIAF at very low-accretion rates. On the other hand, they can naturally be explained by emission from the jets, if the emitting electrons follow a power-law spectral distribution (as is often assumed). The situation remains ambiguous in the case of XTE J1550-564, due to the relatively poorer quality of the data. We discuss the implication of the results.

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