SS433: a massive X-ray binary at advanced evolutionary stage

• Published in: arXiv.org 2019-05
• Main Authors: Cherepashchuk, Anatol, Postnov, Konstantin, Molkov, Sergey, Antokhina, Eleonora, Belinski, Alexander
• Format: Article
• Language: English
• Subjects: Black holes; Broadband; Deposition; Emission; Light curve; Mass transfer; Optical components; Orbital stability; Orbits; Radial velocity; Relativism; Relativistic effects; Stability analysis; X ray binaries; X ray stars
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.1905.02938

INTEGRAL IBIS/ISGRI 18-60 keV observations of SS433 performed in 2003-2011 enabled the hard X-ray phase-resolved orbital and precessional light curves and spectra to be constructed. The spectra can be fitted by a power-law with photon index \(\simeq 3.8\) and remain almost constant while the X-ray flux varies by a factor of a few. This suggests that the hard X-ray emission is produced in an extended quasi-isothermal hot 'corona' surrounding central parts of a supercritical accretion disc. A joint analysis of the broadband 18-60 keV orbital and precessional light curves was performed in the model assuming a significant Roche lobe overfilling by the optical star, up to its filling the outer Lagrangian surface enabling mass loss through the outer Lagrangian L\(_2\) point. From this modeling, the relativistic-to-optical component mass ratio \(q=M_x/M_v\gtrsim0.4\div 0.8\) is estimated. An analysis of the observed long-term stability of the orbital period of SS433 with an account of the recent observations of SS433 by the VLTI GRAVITY interferometer enabled an independent mass ratio estimate \(q>0.6\). This estimate in combination with the radial velocity semi-amplitude for stationary He II emission, \(K_x=168\pm 18\) km/s (Hillwig et al 2004) suggests the optical component mass in SS433 \(M_v>12 M_\odot\). Thus, the mass of the relativistic component in SS433 is \(M_x>7 M_\odot\), which is close to the mean mass of black holes in X-ray binaries (\(\sim 8 M_\odot\)). The large binary mass ratio in SS433 allows us to understand why there is no common envelope in this binary at the secondary mass transfer evolutionary stage and the system remains semi-detached (van den Heuvel et al. 2017). We also discuss unsolved issues and outline prospects for further study of SS433.