1. PS18kh: A New Tidal Disruption Event with a Non-axisymmetric Accretion Disk
- Author
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Pan-Starrs, Asas-Sn, Atlas, Holoien, TWS, Huber, ME, Shappee, BJ, Eracleous, M, Auchettl, K, Brown, JS, Tucker, MA, Chambers, KC, Kochanek, CS, Stanek, KZ, Rest, A, Bersier, D, Post, RS, Aldering, G, Ponder, KA, Simon, JD, Kankare, E, Dong, D, Hallinan, G, Reddy, NA, Sanders, RL, Topping, MW, Bulger, J, Lowe, TB, Magnier, EA, Schultz, ASB, Waters, CZ, Willman, M, Wright, D, Young, DR, Dong, S, Prieto, JL, Thompson, TA, Denneau, L, Flewelling, H, Heinze, AN, Smartt, SJ, Smith, KW, Stalder, B, Tonry, JL, and Weiland, H
- Subjects
accretion accretion disks ,black hole physics ,galaxies: nuclei ,astro-ph.HE ,Astronomical and Space Sciences ,Atomic ,Molecular ,Nuclear ,Particle and Plasma Physics ,Physical Chemistry (incl. Structural) ,Astronomy & Astrophysics - Abstract
We present the discovery of PS18kh, a tidal disruption event discovered at the center of SDSS J075654.53+341543.6 (d ≃ 322 Mpc) by the Pan-STARRS Survey for Transients. Our data set includes pre-discovery survey data from Pan-STARRS, the All-sky Automated Survey for Supernovae, and the Asteroid Terrestrial-impact Last Alert System as well as high-cadence, multiwavelength follow-up data from ground-based telescopes and Swift, spanning from 56 days before peak light until 75 days after. The optical/UV emission from PS18kh is well-fit as a blackbody with temperatures ranging from T ≃ 12,000 K to T ≃ 25,000 K and it peaked at a luminosity of L ≃ 8.8 × 1043 erg s-1. PS18kh radiated E = (3.45 ± 0.22) × 1050 erg over the period of observation, with (1.42 ± 0.20) × 1050 erg being released during the rise to peak. Spectra of PS18kh show a changing, boxy/double-peaked Hα emission feature, which becomes more prominent over time. We use models of non-axisymmetric accretion disks to describe the profile of the Hα line and its evolution. We find that at early times the high accretion rate leads the disk to emit a wind which modifies the shape of the line profile and makes it bell-shaped. At late times, the wind becomes optically thin, allowing the non-axisymmetric perturbations to show up in the line profile. The line-emitting portion of the disk extends from r in ∼ 60r g to an outer radius of r out ∼ 1400r g and the perturbations can be represented either as an eccentricity in the outer rings of the disk or as a spiral arm in the inner disk.
- Published
- 2019