%0 Generic %1 citeulike:13527312 %A Piran, Tsvi %A Svirski, Gilad %A Krolik, Julian %A Cheng, Roseanne M. %A Shiokawa, Hotaka %D 2015 %K imported %T "Circularization" vs. Accretion &\#45;&\#45; What Powers Tidal Disruption Events? %U http://arxiv.org/abs/1502.05792 %X 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, the other half is unbound. To "circularize", i.e., 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 (\~ 10^51 (R/1000R\_g)^-1 erg). Recent numerical simulations (Shiokawa et al., 2015) have revealed that the circularization scale is close to the scale of the most-bound initial orbits, \~ 10^3 M\_BH,6.5^-2/3 R\_g \~ 10^15 M\_BH,6.5^1/3 cm from the black hole, and the corresponding circularization energy dissipation rate is \$10^44 M\_BH,6.5^-1/6\$\~erg/s. We suggest that the energy liberated during circularization, rather then energy liberated by accretion onto the black hole, powers the observed optical TDE candidates (e.g.Arcavi et al. 2014). 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 circularization than in terms of accretion.

@misc{citeulike:13527312, abstract = {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, the other half is unbound. To "circularize", i.e., 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 (\~{} 10^{51} (R/1000R\_g)^{-1} erg). Recent numerical simulations (Shiokawa et al., 2015) have revealed that the circularization scale is close to the scale of the most-bound initial orbits, \~{} 10^3 M\_{BH,6.5}^{-2/3} R\_g \~{} 10^{15} M\_{BH,6.5}^{1/3} cm from the black hole, and the corresponding circularization energy dissipation rate is \$\sim 10^{44} M\_{BH,6.5}^{-1/6}\$\~{}erg/s. We suggest that the energy liberated during circularization, rather then energy liberated by accretion onto the black hole, powers the observed optical TDE candidates (e.g.Arcavi et al. 2014). 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 circularization than in terms of accretion.}, added-at = {2019-03-25T08:20:55.000+0100}, archiveprefix = {arXiv}, author = {Piran, Tsvi and Svirski, Gilad and Krolik, Julian and Cheng, Roseanne M. and Shiokawa, Hotaka}, biburl = {https://www.bibsonomy.org/bibtex/2728fe71f8e8a02d325ec51dc1eb04cd6/ericblackman}, citeulike-article-id = {13527312}, citeulike-linkout-0 = {http://arxiv.org/abs/1502.05792}, citeulike-linkout-1 = {http://arxiv.org/pdf/1502.05792}, day = 20, eprint = {1502.05792}, interhash = {9e199d9aa8362877fcb10f3515c90ccf}, intrahash = {728fe71f8e8a02d325ec51dc1eb04cd6}, keywords = {imported}, month = feb, posted-at = {2015-02-25 08:46:13}, priority = {2}, timestamp = {2019-03-25T08:20:55.000+0100}, title = {{"Circularization" vs. Accretion \&\#45;\&\#45; What Powers Tidal Disruption Events?}}, url = {http://arxiv.org/abs/1502.05792}, year = 2015 }