TY - JOUR
T1 - DISK FORMATION VERSUS DISK ACCRETION - WHAT POWERS TIDAL DISRUPTION EVENTS?
AU - Piran, Tsvi
AU - Svirski, Gilad
AU - Krolik, Julian
AU - Cheng, Roseanne M.
AU - Shiokawa, Hotaka
N1 - Publisher Copyright:
© 2015. The American Astronomical Society. All rights reserved.
PY - 2015/6/20
Y1 - 2015/6/20
N2 - A tidal disruption event (TDE) takes place when a star passes near enough to a massive black hole to be disrupted. About half the star's matter is given elliptical trajectories with large apocenter distances, and the other half is unbound. To form an accretion flow, the bound matter must lose a significant amount of energy, with the actual amount depending on the characteristic scale of the flow measured in units of the black hole's gravitational radius (∼1051(R/1000Rg)-1 erg). Recent numerical simulations have revealed that the accretion flow scale is close to the scale of the most bound initial orbits, ∼103MBH,6.5-2/3Rg ∼ 1015MBH,6.51/3 cm from the black hole, and the corresponding energy dissipation rate is ∼1044MBH,6.5-1/6erg s-1. We suggest that the energy liberated during the formation of the accretion disk, rather than the energy liberated by subsequent accretion onto the black hole, powers the observed optical TDE candidates. The observed rise times, luminosities, temperatures, emission radii, and line widths seen in these TDEs are all more readily explained in terms of heating associated with disk formation rather than in terms of accretion.
AB - A tidal disruption event (TDE) takes place when a star passes near enough to a massive black hole to be disrupted. About half the star's matter is given elliptical trajectories with large apocenter distances, and the other half is unbound. To form an accretion flow, the bound matter must lose a significant amount of energy, with the actual amount depending on the characteristic scale of the flow measured in units of the black hole's gravitational radius (∼1051(R/1000Rg)-1 erg). Recent numerical simulations have revealed that the accretion flow scale is close to the scale of the most bound initial orbits, ∼103MBH,6.5-2/3Rg ∼ 1015MBH,6.51/3 cm from the black hole, and the corresponding energy dissipation rate is ∼1044MBH,6.5-1/6erg s-1. We suggest that the energy liberated during the formation of the accretion disk, rather than the energy liberated by subsequent accretion onto the black hole, powers the observed optical TDE candidates. The observed rise times, luminosities, temperatures, emission radii, and line widths seen in these TDEs are all more readily explained in terms of heating associated with disk formation rather than in terms of accretion.
KW - accretion, accretion disks
KW - black hole physics
KW - galaxies: nuclei
KW - stars: black holes
UR - http://www.scopus.com/inward/record.url?scp=84934902504&partnerID=8YFLogxK
U2 - 10.1088/0004-637X/806/2/164
DO - 10.1088/0004-637X/806/2/164
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AN - SCOPUS:84934902504
SN - 0004-637X
VL - 806
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 164
ER -