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arxiv: 2201.02649 · v2 · pith:THP5HEUEnew · submitted 2022-01-07 · 🌌 astro-ph.HE · astro-ph.CO· astro-ph.SR

Systematic light curve modelling of TDEs: statistical differences between the spectroscopic classes

classification 🌌 astro-ph.HE astro-ph.COastro-ph.SR
keywords tde-htdeseventsclassesdifferencesspectroscopicencountersfind
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With the sample of observed tidal disruption events (TDEs) now reaching several tens, distinct spectroscopic classes have emerged: TDEs with only hydrogen lines (TDE-H), only helium lines (TDE-He), or hydrogen in combination with He II and often N III/O III (TDE-H+He). Here we model the light curves of 32 optically-bright TDEs using the Modular Open Source Fitter for Transients (MOSFiT) to estimate physical and orbital properties, and look for statistical differences between the spectroscopic classes. For all types, we find a shallow distribution of star masses, compared to a typical initial mass function, between $\sim 0.1-1$ M$_\odot$, and no TDEs with very deep ($\beta \gg 1$) encounters. Our main result is that TDE-H events appear to come from less complete disruptions (and possibly lower SMBH masses) than TDE-H+He, with TDE-He events fully disrupted. We also find that TDE-H events have more extended photospheres, in agreement with recent literature, and argue that this could be a consequence of differences in the self-intersection radii of the debris streams. Finally, we identify an approximately linear correlation between black hole mass and radiative efficiency. We suggest that TDE-H may be powered by collision-induced outflows at relatively large radii, while TDE-H+He could result from prompt accretion disks, formed more efficiently in closer encounters around more massive SMBHs.

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Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. The Light Curve of Wind-Reprocessed Tidal Disruption Events

    astro-ph.HE 2026-06 unverdicted novelty 5.0

    Radiation hydrodynamic simulations of wind-reprocessed TDEs reveal a ~3-week offset between optical/UV and bolometric light curve peaks due to the buildup time of the reprocessing layer.