TY - JOUR
T1 - Implications from Late-time X-Ray Detections of Optically Selected Tidal Disruption Events
T2 - State Changes, Unification, and Detection Rates
AU - Jonker, P. G.
AU - Stone, N. C.
AU - Generozov, A.
AU - Velzen, S. Van
AU - Metzger, B.
N1 - Publisher Copyright:
© 2020. The American Astronomical Society. All rights reserved.
PY - 2020/2/1
Y1 - 2020/2/1
N2 - 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 × 1040 and 3 × 1042 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).
AB - 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 × 1040 and 3 × 1042 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).
UR - http://www.scopus.com/inward/record.url?scp=85081395023&partnerID=8YFLogxK
U2 - 10.3847/1538-4357/ab659c
DO - 10.3847/1538-4357/ab659c
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AN - SCOPUS:85081395023
SN - 0004-637X
VL - 889
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 166
ER -