Issue |
A&A
Volume 697, May 2025
|
|
---|---|---|
Article Number | A229 | |
Number of page(s) | 17 | |
Section | Astrophysical processes | |
DOI | https://doi.org/10.1051/0004-6361/202453538 | |
Published online | 23 May 2025 |
Evolution of the Comptonizing medium of the black-hole candidate Swift J1727.8–1613 along the hard to hard-intermediate state transition using NICER
1
Observatoire Astronomique de Strasbourg, Université de Strasbourg, CNRS, 11 rue de l’Université, F-67000 Strasbourg, France
2
Kapteyn Astronomical Institute, University of Groningen, PO BOX 800, Groningen NL-9700 AV, The Netherlands
3
Instituto Argentino de Radioastronomí (CCT La Plata, CONICET; CICPBA; UNLP), C.C.5, (1894) Villa Elisa, Buenos Aires, Argentina
⋆ Corresponding authors: rawat@unistra.fr, mariano@astro.rug.nl
Received:
20
December
2024
Accepted:
5
April
2025
We analyse the properties of the Comptonizing medium in the black-hole X-ray binary Swift J1727.8−1613 using the time-dependent Comptonization model vkompth, applied to NICER observations of type-C QPOs in the hard and hard-intermediate states. During the 2023 outburst of the source, we measure the RMS and phase lags of the QPO across 45 observations as the QPO frequency, νQPO, evolves from ∼0.3 Hz to ∼7 Hz. By simultaneously fitting the time-averaged spectrum of the source and the RMS and lag spectra of the QPO, we derive the evolution of the disc and corona parameters. At νQPO = 0.34 Hz, the QPO phase lags are hard, with 10 keV photons lagging 0.5 keV photons by ∼0.5 rad. As νQPO increases, the lags for the same energy bands decrease, reaching near zero at νQPO∼1.2 Hz, and then reverse to soft lags of ∼−1.1 rad at νQPO∼7 Hz. Initially, the inner radius of the accretion disc is truncated at ∼30−40Rg (assuming a 10 solar-mass black hole) and, as the QPO frequency increases, the truncation radius decreases down to ∼10Rg. Initially, two coronas of sizes of ∼6.5×103 km and ∼2×103 km, extend over the disc and are illuminated by different regions of the disk. As the QPO frequency increases, both the coronas shrink to ∼2×103 km at νQPO = 2.5 Hz. Following a data gap, one corona expands again, peaking at a size of ∼2×104 km. We interpret the evolution of the coronal size in the context of accompanying radio observations, discussing its implications for the interplay between the corona and the jet.
Key words: accretion, accretion disks / black hole physics / methods: data analysis / stars: black holes / X-rays: binaries / X-rays: individuals: Swift J1727.8–1613
© The Authors 2025
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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