Hostname: page-component-78c5997874-lj6df Total loading time: 0 Render date: 2024-11-15T20:53:40.805Z Has data issue: false hasContentIssue false

Instabilities in the Gamma Ray Burst central engine. What makes the jet variable?

Published online by Cambridge University Press:  24 February 2011

Agnieszka Janiuk
Affiliation:
Center for Theoretical Physics, Polish Academy of Sciences, Al. Lotnikow 32/46, 02-668 Warsaw, Poland
Ye-Fei Yuan
Affiliation:
Department of Astronomy, University of Science and Technology of China, Chinese Academy of Sciences, Hefei, Anhui 230026, P.R. China
Rosalba Perna
Affiliation:
JILA and Department of Astrophysical and Planetary Sciences, University of Colorado, Boulder, CO 80309USA
Tiziana Di Matteo
Affiliation:
Physics Department, Carnegie Mellon University, 5000 Forbes Avenue, Pittsburgh, PA 15232
Rights & Permissions [Opens in a new window]

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

Both types of long and short gamma ray bursts involve a stage of a hyper-Eddington accretion of hot and dense plasma torus onto a newly born black hole. The prompt gamma ray emission originates in jets at some distance from this ‘central engine’ and in most events is rapidly variable, having a form of sipkes and subpulses. This indicates at the variable nature of the engine itself, for which a plausible mechanism is an internal instability in the accreting flow. We solve numerically the structure and evolution of the neutrino-cooled torus. We take into account the detailed treatment of the microphysics in the nuclear equation of state that includes the neutrino trapping effect. The models are calculated for both Schwarzschild and Kerr black holes. We find that for sufficiently large accretion rates (>~10M s−1 for non-rotating black hole, and >~1M s−1 for rotating black hole, depending on its spin), the inner regions of the disk become opaque, while the helium nuclei are being photodissociated. The sudden change of pressure in this region leads to the development of a viscous and thermal instability, and the neutrino pressure acts similarly to the radiation pressure in sub-Eddington disks. In the case of rapidly rotating black holes, the instability is enhanced and appears for much lower accretion rates. We also find the important and possibly further destabilizing role of the energy transfer from the rotating black hole to the torus via the magnetic coupling.

Type
Contributed Papers
Copyright
Copyright © International Astronomical Union 2011

References

Chen, W. X. & Beloborodov, A. 2007, ApJ, 657, 383CrossRefGoogle Scholar
Di Matteo, T., Perna, R., Narayan, R. 2002, ApJ, 579, 706Google Scholar
Fender, R. P., Gallo, E., Russell, D. 2010, MNRAS, 406, 1425Google Scholar
Janiuk, A., Czerny, B., Siemiginowska, A. 2002, ApJ, 576, 908CrossRefGoogle Scholar
Janiuk, A., Perna, R., Di Matteo, T., Czerny, B. 2004, MNRAS, 355, 950CrossRefGoogle Scholar
Janiuk, A., Yuan, Y.-F., Perna, R., Di Matteo, T. 2007, ApJ, 664, 1011CrossRefGoogle Scholar
Janiuk, A., Moderski, R., Proga, D. 2008, ApJ, 687, 433CrossRefGoogle Scholar
Janiuk, A., Yuan, Y.-F., 2010, A&A, 509, 55Google Scholar
Lei, W. H., Wang, D. X., Zhang, L., et al. 2009, ApJ, 700, 1970CrossRefGoogle Scholar
MacFadyen, A., Woosley, S. E. 1999, ApJ, 524, 262CrossRefGoogle Scholar
Perna, R., Armitage, P., Zhang, B. 2006, ApJ 636, L29Google Scholar
Piran, T. 2005, Rev. Mod. Phys. 76, 1143CrossRefGoogle Scholar
Popham, R., Woosley, S. E., Fryer, C. 1999, ApJ, 518, 356CrossRefGoogle Scholar
Wang, D. X., Xiao, K., Lei, W.-H., 2002, MNRAS, 335, 655Google Scholar