2018/03/31 by Giacomo Fragione, Nathan W. C. Leigh, Nathan Leigh · 32 citations
Physics and Astronomy · #Astronomy #Astrophysical Phenomena and Observations #Astrophysics #Galactic Center #Galaxies: Formation, Evolution, Phenomena #Galaxy #Physics #Stars #Stellar, planetary, and galactic studies #Supermassive black hole #astro-ph.GA #astro-ph.HE
paper · pdf · doi:10.1093/mnras/sty1600
published in Monthly Notices of the Royal Astronomical Society 479(3), 3181-3188 (Oxford University Press) · 9 pages, 7 figures, 2 Tables, MNRAS, Volume 479, Issue 3, p.3181-3188
openalex created_date 2018/04/06 · openalex publication_date 2018/06/14 · arxiv created 2018/08/19 · arxiv updated 2018/08/21 · openalex updated_date 2026/08/05
Stars passing too close to a supermassive black hole (SMBH) can produce tidal disruption events (TDEs). Since the resulting stellar debris can produce an electromagnetic flare, TDEs are believed to probe the presence of single SMBHs in galactic nuclei, which otherwise remain dark. In this paper, we show how stars orbiting an intermediate-mass black hole (IMBH) secondary are perturbed by an SMBH primary. We find that the evolution of the stellar orbits are severely affected by the primary SMBH due to secular effects and stars orbiting with high inclinations with respect to the SMBH–IMBH orbital plane end their lives as TDEs due to Kozai–Lidov oscillations, hence illuminating the secondary SMBH/IMBH. Above a critical SMBH mass of ≈1.15 × 108 M⊙, no TDE can occur for typical stars in an old stellar population since the Schwarzschild radius exceeds the tidal disruption radius. Consequently, any TDEs due to such massive SMBHs will remain dark. It follows that no TDEs should be observed in galaxies with bulges more massive than ≈4.15 × 1010 M⊙, unless a lower mass secondary SMBH or IMBH is also present. The secular mechanism for producing TDEs considered here therefore offers a useful probe of SMBH–SMBH/IMBH binarity in the most massive galaxies. We further show that the TDE rate can be ≈10−4–10−3 yr−1, and that most TDEs occur on ≈0.5 Myr. Finally, we show that stars may be ejected with velocities up to thousands of km s−1, which could contribute to the observed population of galactic hypervelocity stars.