Jet precession driven by neutrino-cooled disk for gamma-ray bursts

被引:52
|
作者
Liu, T. [1 ]
Liang, E. -W. [2 ]
Gu, W. -M. [3 ,4 ]
Zhao, X. -H. [5 ,6 ]
Dai, Z. -G. [1 ]
Lu, J. -F. [3 ,4 ]
机构
[1] Nanjing Univ, Dept Astron, Nanjing 210093, Jiangsu, Peoples R China
[2] Guangxi Univ, Dept Phys, Nanning 530004, Guangxi, Peoples R China
[3] Xiamen Univ, Dept Phys, Xiamen 361005, Fujian, Peoples R China
[4] Xiamen Univ, Inst Theoret Phys & Astrophys, Xiamen 361005, Fujian, Peoples R China
[5] Chinese Acad Sci, Yunnan Observ, Natl Astron Observ, Kunming 650011, Yunnan, Peoples R China
[6] Chinese Acad Sci, Key Lab Struct & Evolut Celestial Bodies, Kunming 650011, Yunnan, Peoples R China
基金
中国博士后科学基金; 中国国家自然科学基金;
关键词
accretion: accretion disks; black hole physics; gamma ray burst: general; ACCRETION DISKS; DOMINATED ACCRETION; LIGHT CURVES; BLACK-HOLES; MODELS; LUMINOSITY; EVOLUTION; LONG; STAR; GRB-980425;
D O I
10.1051/0004-6361/200913447
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Aims. A model of jet precession driven by a neutrino-cooled disk around a spinning black hole is presented to explain the temporal structure and spectral evolution of gamma-ray bursts (GRBs). Methods. The differential rotation of the outer part of a neutrino-dominated accretion disk may result in precession of the inner part of the disk and the central black hole, hence driving a precessed jet via neutrino annihilation around the inner part of the disk. Results. Both analytic and numeric results for our model are presented. Our calculations show that a black-hole, accretion-disk system with the black hole mass M similar or equal to 3.66 M-circle dot, accretion rate. M similar or equal to 0.54 M-circle dot s(-1), spin parameter a = 0.9, and viscosity parameter alpha = 0.01 may drive a precessed jet with period P = 1 s and luminosity L = 10(51) erg s(-1), corresponding to the scenario for long GRBs. A precessed jet with P = 0.1 s and L = 10(50) erg s(-1) may be powered by a system with M similar or equal to 5.59 M-circle dot, M similar or equal to 0.74 M similar or equal to s(-1), a = 0.1, and alpha = 0.01, and is possibly responsible for the short GRBs. Both the temporal and spectral evolution in GRB pulse may be explained with our model. Conclusions. GRB central engines most likely power a precessed jet driven by a neutrino-cooled disk. The global GRB lightcurves thus could be modulated by the jet precession during the accretion timescale of the GRB central engine. Both the temporal and spectral evolution in GRB pulse may stem from a viewing effect of the jet precession.
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页数:5
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