The peculiar spectral evolution of the new X-ray transient MAXI J0637–430

Author:

Ma R C12ORCID,Soria R34,Tao L1,Zhang W12,Qu J L1,Zhang S N12,Zhang L1ORCID,Qiao E L25,Zhao S J12,Ge M Y1,Li X B1,Huang Y1,Song L M1ORCID,Zhang S1,Bu Q C6ORCID,Wang Y N7,Ma X1,Jia S M1

Affiliation:

1. Key Laboratory of Particle Astrophysics, Institute of High Energy Physics, Chinese Academy of Sciences , Beijing 100049, People’s Republic of China

2. University of Chinese Academy of Sciences, Chinese Academy of Sciences , Beijing 100049, People’s Republic of China

3. College of Astronomy and Space Sciences, University of the Chinese Academy of Sciences , Beijing 100049, People’s Republic of China

4. Sydney Institute for Astronomy , School of Physics A28, The University of Sydney, Sydney, NSW 2006, Australia

5. Key Laboratory of Space Astronomy and Technology, National Astronomical Observatories, Chinese Academy of Sciences , Beijing 100012, People’s Republic of China

6. Institut für Astronomie und Astrophysik, Kepler Center for Astro and Particle Physics, Eberhard Karls Universität , D-72076 Tübingen, Germany

7. Physics and Astronomy, University of Southampton , Southampton, Hampshire SO17 1BJ, UK

Abstract

ABSTRACT We studied the transient Galactic black hole candidate MAXI J0637−430 with data from Insight-HXMT, Swift, and XMM–Newton. The broad-band X-ray observations from Insight-HXMT help us constrain the power-law component. MAXI J0637–430 is located at unusually high Galactic latitude; if it belongs to the Galactic thick disc, we suggest a most likely distance ≲7 kpc. Compared with other black hole transients, MAXI J0637–430 is also unusual for other reasons: a fast transition to the thermal dominant state at the start of the outburst; a low peak temperature and luminosity (we estimate them at ≈0.7 keV and ≲0.1 times Eddington, respectively); a short decline time-scale; a low soft-to-hard transition luminosity (≲0.01 times Eddington). We argue that such properties are consistent with a small binary separation, short binary period (P ∼ 2 h), and low-mass donor star (M2 ∼ 0.2 M⊙). Moreover, spectral modelling shows that a single disc blackbody component is not a good fit to the thermal emission. Soft spectral residuals, and deviations from the standard $L_{\rm disc} \propto T_{\rm in}^4$ relation, suggest the need for a second thermal component. We propose and discuss various scenarios for such component, in addition to those presented in previous studies of this source. For example, a gap in the accretion disc between a hotter inner ring near the innermost stable orbit, and a cooler outer disc. Another possibility is that the second thermal component is the thermal plasma emission from an ionized outflow.

Funder

CNSA

Chinese Academy of Sciences

CAS

National Key Research and Development Program of China

National Natural Science Foundation of China

IHEP

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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