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Implications from Late-time X-Ray Detections of Optically Selected Tidal Disruption Events: State Changes, Unification, and Detection Rates

P. G. JonkerDepartment of Astrophysics/IMAPP, Radboud University, P.O. Box 9010, 6500 GL, Nijmegen, The NetherlandsNicholas C. StoneDepartment of Astronomy, University of Maryland, Stadium Drive, College Park, MD 20742-2421, USAAleksey GenerozovDepartment of Physics, Department of Astronomy, and Columbia Astrophysics Laboratory, Columbia University, New York, NY 10027, USASjoert van VelzenCenter for Cosmology and Particle Physics, New York University, New York, NY 10003, USABrian D. MetzgerDepartment of Physics, Department of Astronomy, and Columbia Astrophysics Laboratory, Columbia University, New York, NY 10027, USA
2020en
ABI

Аннотация

Abstract We present Chandra X-ray observations of four optically selected tidal disruption events (TDEs) obtained 4–9 yr after discovery. Three sources were detected with luminosities between 9 × 10 40 and 3 × 10 42 erg s −1 . The spectrum of PTF09axc is consistent with a power law of index 2.5 ± 0.1, whereas the spectrum of PTF09ge is very soft. The power-law spectrum of PTF09axc and prior literature findings provide evidence that TDEs transition from an early-time soft state to a late-time hard state many years after disruption. We propose that the time to peak luminosity for optical and X-ray emission may differ substantially in TDEs, with X-rays being produced or becoming observable later. This delay helps explain the differences in observed properties such as L opt / L X of optically and X-ray-selected TDEs. We update TDE rate predictions for the eROSITA instrument: it ranges from 3 to 990 yr −1 , depending sensitively on the distribution of black hole spins and the time delay between disruption and peak X-ray brightness. We further predict an asymmetry in the number of retrograde and prograde disks in samples of optically and X-ray-selected TDEs. The details of the observational biases can contribute to observed differences between optically and X-ray-selected TDEs (with optically selected TDEs being fainter in X-rays for retrograde TDE disks).

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