Simulations of ultrarelativistic magnetodynamic jets from gamma-ray burst engines

被引:223
作者
Tchekhovskoy, Alexander [1 ]
McKinney, Jonathan C. [2 ]
Narayan, Ramesh [1 ]
机构
[1] Harvard Smithsonian Ctr Astrophys, Inst Theory & Computat, Cambridge, MA 02138 USA
[2] Stanford Univ, Kavli Inst Particle Astrophys & Cosmol, Stanford, CA 94309 USA
关键词
accretion; accretion discs; black hole physics; hydrodynamics; MHD; methods : numerical; galaxies : jets;
D O I
10.1111/j.1365-2966.2008.13425.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Long-duration gamma-ray bursts (GRBs) require an engine capable of driving a jet of plasma to ultrarelativistic bulk Lorentz factors of up to several hundred and into narrow opening angles of a few degrees. We use global axisymmetric stationary solutions of magnetically dominated (force-free) ultrarelativistic jets to test whether the popular magnetic-driving paradigm can generate the required Lorentz factors and opening angles. Our global solutions are obtained via time-dependent relativistic ideal magnetodynamical numerical simulations which follow the jet from the central engine to beyond six orders of magnitude in radius. Our model is primarily motivated by the collapsar model, in which a jet is produced by a spinning black hole or neutron star and then propagates through a massive stellar envelope. We find that the size of the pre-supernova progenitor star and the radial profile of pressure inside the star determine the terminal Lorentz factor and opening angle of the jet. At the radius where the jet breaks out of the star, our well-motivated fiducial model generates a Lorentz factor gamma similar to 400 and a half-opening angle theta(j) similar to 2 degrees, consistent with observations of many long-duration GRBs. Other models with slightly different parameters give gamma in the range 100-5000 and theta(j) from 0 degrees.1 to 10 degrees, thus reproducing the range of properties inferred for GRB jets. A potentially observable feature of some of our solutions is that the maximum Poynting flux in the jet is found at theta similar to theta(j) with the jet power concentrated in a hollow cone, while the maximum in the Lorentz factor occurs at an angle theta substantially smaller than theta(j) also in a hollow cone. We derive approximate analytical formulae for the radial and angular distribution of. and the radial dependence of theta(j). These formulae reproduce the simulation results and allow us to predict the outcome of models beyond those simulated. We also briefly discuss applications to active galactic nuclei, X-ray binaries and short-duration GRBs.
引用
收藏
页码:551 / 572
页数:22
相关论文
共 121 条
[91]   GAMMA-RAY BURSTS AS THE DEATH THROES OF MASSIVE BINARY STARS [J].
NARAYAN, R ;
PACZYNSKI, B ;
PIRAN, T .
ASTROPHYSICAL JOURNAL, 1992, 395 (02) :L83-L86
[92]   ADVECTION-DOMINATED ACCRETION - A SELF-SIMILAR SOLUTION [J].
NARAYAN, R ;
YI, I .
ASTROPHYSICAL JOURNAL, 1994, 428 (01) :L13-L13
[93]   Advection-dorninated accretion and the black hole event horizon [J].
Narayan, Ramesh ;
McClintock, Jeffrey E. .
NEW ASTRONOMY REVIEWS, 2008, 51 (10-12) :733-751
[94]   Self-similar force-free wind from an accretion disc [J].
Narayan, Ramesh ;
McKinney, Jonathan C. ;
Farmer, Alison J. .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2007, 375 (02) :548-566
[95]   RELATIVISTIC CENTRIFUGAL WINDS [J].
OKAMOTO, I .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1978, 185 (01) :69-107
[96]   MAGNETIC BRAKING BY A STELLAR WIND .4. EFFECT OF DIFFERENT POLOIDAL FIELD STRUCTURES [J].
OKAMOTO, I .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1974, 166 (03) :683-701
[97]   Are gamma-ray bursts in star-forming regions? [J].
Paczynski, B .
ASTROPHYSICAL JOURNAL, 1998, 494 (01) :L45-L48
[98]  
Piran T, 2004, REV MOD PHYS, V76, P1143, DOI 10.1103/RevModPhys.76.1143
[99]   Hyperaccreting black holes and gamma-ray bursts [J].
Popham, R ;
Woosley, SE ;
Fryer, C .
ASTROPHYSICAL JOURNAL, 1999, 518 (01) :356-374
[100]   The dynamics and light curves of beamed gamma-ray burst afterglows [J].
Rhoads, JE .
ASTROPHYSICAL JOURNAL, 1999, 525 (02) :737-749