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Modeling X-ray reflection spectra from returning radiation: application to 4U 1630$-$47

Kostas KourmpetisInstitut für Astronomie und Astrophysik , Eberhard-Karls Universität Tübingen , Sand 1 , 72076 Tübingen , GermanyShafqat RiazTheoretical Astrophysics , IAAT , Eberhard-Karls Universität Tübingen , D-72076 Tübingen , GermanyH. LiuInstitut für Astronomie und Astrophysik , Eberhard-Karls Universität Tübingen , Sand 1 , 72076 Tübingen , GermanyTemurbek MirzaevCenter for Astronomy and Astrophysics , Center for Field Theory and Particle Physics and Department of Physics , Fudan University , 200438 Shanghai , ChinaCosimo BambiCenter for Astronomy and Astrophysics , Center for Field Theory and Particle Physics and Department of Physics , Fudan University , 200438 Shanghai , ChinaDebtroy DasCenter for Astronomy and Astrophysics , Center for Field Theory and Particle Physics and Department of Physics , Fudan University , 200438 Shanghai , ChinaJiachen JiangDepartment of Physics , University of Warwick , Coventry CV4 7AL , UKKostas D. KokkotasTheoretical Astrophysics , IAAT , Eberhard-Karls Universität Tübingen , D-72076 Tübingen , GermanyA. SantangeloInstitut für Astronomie und Astrophysik , Eberhard-Karls Universität Tübingen , Sand 1 , 72076 Tübingen , Germany
2026
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Annotatsiya

Returning radiation is thought to play a key role in disk illumination of black hole X-ray binaries in the high-soft state, yet it has not been fully incorporated into XSPEC reflection models. We present a new table model for reflection spectroscopy that, for the first time, self-consistently accounts for the returning radiation. To isolate this effect, we adopt the standard disk-corona configuration but disable the corona, allowing the reflection spectrum to be produced solely by self-irradiation of the disk. Applying our model to the black hole X-ray binary 4U 1630$-$47, we report a rapidly spinning black hole ($a_* \sim 0.99$), a disk inclination of $i \sim 53^\circ$, a mass accretion rate of $\dot{M}_{\rm BH} \sim 15\% \, {\rm \dot{M}_{Edd}}$, and an electron density of $n_{\rm e} \sim 10^{21} \,\mathrm{cm^{-3}}$ to reproduce the observed reflection features. The model also yields a source distance of $D\sim 8.2 \, {\rm kpc}$, slightly below the commonly adopted value of $10 \, {\rm kpc}$ in the literature. Compared to the widely used relxillNS, our model naturally produces a harder high-energy reflection spectrum, fitting the data without invoking a Comptonized component.

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