TY - JOUR
T1 - Relativistic MHD simulations of core-collapse GRB jets
T2 - 3D instabilities and magnetic dissipation
AU - Bromberg, Omer
AU - Tchekhovskoy, Alexander
N1 - Funding Information:
We thank R. Barniol Duran, E. Blackman, D. Giannios, D. Lazzati, H. Li, Y. Lyubarsky, J. McKinney, R. Narayan, K. Parfrey, A. Philippov, S. Phinney, E. Quataert, F. Ryde, A. Spitkovsky, N. Stone, and S. Woosley for discussions that helped us to improve this work. OB acknowledges support from the Lyman Spitzer Jr Fellowship, awarded by the Department of Astrophysical Sciences at Princeton University and the Max-Planck/Princeton Center for Plasma Physics which facilitated this work. AT was supported by NASAthrough Einstein Postdoctoral Fellowship grant number PF3- 140115 awarded by the Chandra X-ray Center, which is operated by the Smithsonian Astrophysical Observatory for NASA under contract NAS8-03060, and NSF through an XSEDE computational time allocation TG-AST100040 on NICS Kraken, Nautilus, TACC Stampede, Maverick, and Ranch. AT thanks Skyhouse for their hospitality and fostering productive discussions that helped us refine the understanding of the factors that control the large-scale jet morphology. The simulations presented in this work also used computational resources supported by the PICSciE-OIT High Performance Computing Center and Visualization Laboratory, and the Savio cluster provided by UCB.
PY - 2016
Y1 - 2016
N2 - Relativistic jets are associated with extreme astrophysical phenomena, like the core collapse of massive stars in gamma-ray bursts (GRBs) and the accretion on to supermassive black holes in active galactic nuclei. It is generally accepted that these jets are powered electromagnetically, by the magnetized rotation of a central compact object (black hole or neutron star). However, how the jets produce the observed emission and survive the propagation for many orders of magnitude in distance without being disrupted by current-driven instabilities is the subject of active debate. We carry out time-dependent 3D relativistic magnetohydrodynamic (MHD) simulations of relativistic, Poynting-flux-dominated jets. The jets are launched self-consistently by the rotation of a strongly magnetized central object. This determines the natural degree of azimuthal magnetic field winding, a crucial factor that controls jet stability. We find that the jets are susceptible to two types of instability: (i) a global, external kink mode that grows on long time-scales. It bodily twists the jet, reducing its propagation velocity. We show analytically that in flat density profiles, like the ones associated with galactic cores, the external mode grows and may stall the jet. In the steep profiles of stellar envelopes the external kink weakens as the jet propagates outward. (ii) a local, internal kink mode that grows over short time-scales and causes small-angle magnetic reconnection and conversion of about half of the jet electromagnetic energy flux into heat.We suggest that internal kink instability is the main dissipation mechanism responsible for powering GRB prompt emission.
AB - Relativistic jets are associated with extreme astrophysical phenomena, like the core collapse of massive stars in gamma-ray bursts (GRBs) and the accretion on to supermassive black holes in active galactic nuclei. It is generally accepted that these jets are powered electromagnetically, by the magnetized rotation of a central compact object (black hole or neutron star). However, how the jets produce the observed emission and survive the propagation for many orders of magnitude in distance without being disrupted by current-driven instabilities is the subject of active debate. We carry out time-dependent 3D relativistic magnetohydrodynamic (MHD) simulations of relativistic, Poynting-flux-dominated jets. The jets are launched self-consistently by the rotation of a strongly magnetized central object. This determines the natural degree of azimuthal magnetic field winding, a crucial factor that controls jet stability. We find that the jets are susceptible to two types of instability: (i) a global, external kink mode that grows on long time-scales. It bodily twists the jet, reducing its propagation velocity. We show analytically that in flat density profiles, like the ones associated with galactic cores, the external mode grows and may stall the jet. In the steep profiles of stellar envelopes the external kink weakens as the jet propagates outward. (ii) a local, internal kink mode that grows over short time-scales and causes small-angle magnetic reconnection and conversion of about half of the jet electromagnetic energy flux into heat.We suggest that internal kink instability is the main dissipation mechanism responsible for powering GRB prompt emission.
KW - Galaxies: jets
KW - Gamma-ray burst: general
KW - Quasars: general
KW - Stars: magnetars
KW - Stars: magnetic field
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U2 - 10.1093/mnras/stv2591
DO - 10.1093/mnras/stv2591
M3 - Article
AN - SCOPUS:84960800759
VL - 456
SP - 1739
EP - 1760
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
SN - 0035-8711
IS - 2
ER -