The comptonizing medium of the black hole X-ray binary MAXI J1535−571 through type-C quasi-periodic oscillations

Author:

Rawat Divya1ORCID,Méndez Mariano2,García Federico234ORCID,Altamirano Diego5,Karpouzas Konstantinos25ORCID,Zhang Liang5ORCID,Alabarta Kevin25ORCID,Belloni Tomaso M6,Jain Pankaj7,Bellavita Candela4

Affiliation:

1. Inter-University Center for Astronomy and Astrophysics , Ganeshkhind, Pune 411007, India

2. Kapteyn Astronomical Institute, University of Groningen , PO BOX 800, Groningen NL-9700 AV, the Netherlands

3. Instituto Argentino de Radioastronomía (CCT La Plata, CONICET; CICPBA; UNLP) , C.C.5, (1894) Villa Elisa, Buenos Aires, Argentina

4. Facultad de Ciencias Astronómicas y Geofísicas, Universidad Nacional de La Plata , Paseo del Bosque, B1900FWA La Plata, Argentina

5. School of Physics and Astronomy, University of Southampton , Southampton SO17 1BJ, UK

6. INAF – Osservatorio Astronomico di Brera , via E. Bianchi 46, I-23807, Merate, Italy

7. Department of physics, IIT Kanpur , Kanpur, Uttar Pradesh 208016, India

Abstract

ABSTRACT We present a detailed spectral and temporal analysis of the black hole candidate MAXI J1535−571 using NICER observations in 2017 September and October. We focus specifically on observations in the hard-intermediate state when the source shows type-C quasi-periodic oscillations (QPOs). We fitted the time-averaged spectrum of the source and the rms and phase-lag spectra of the QPO with a one-component time-dependent Comptonization model. We found that the corona contracts from ∼104–3× 10 3 km as the QPO frequency increases from ∼ 1.8–9.0 Hz. The fits suggest that the system would consist of two coronas, a small one that dominates the time-averaged spectrum and a larger one, possibly the jet, that dominates the rms and lag spectra of the QPO. We found a significant break in the relation between the spectral parameters of the source and the properties of the QPO, including its lag spectra, with QPO frequency. The change in the relations happens when the QPO frequency crosses a critical frequency ν c ≈ 3.0 Hz. Interestingly, the QPO reaches this critical frequency simultaneously as the radio emission from the jet in this source is quenched.

Funder

NWO

CONICET

ANPCyT

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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