How to Turn Jets into Cylinders near Supermassive Black Holes in 3D General Relativistic Magnetohydrodynamic Simulations

被引:2
|
作者
Rohoza, Valeriia [1 ]
Lalakos, Aretaios [1 ]
Paik, Max [1 ,2 ]
Chatterjee, Koushik [3 ,4 ]
Liska, Matthew [5 ,6 ]
Tchekhovskoy, Alexander [1 ]
Gottlieb, Ore [1 ,7 ,8 ,9 ]
机构
[1] Northwestern Univ, Ctr Interdisciplinary Explorat & Res Astrophys CIE, Phys & Astron, Evanston, IL 60202 USA
[2] NYU, Courant Inst Math Sci, New York, NY 10011 USA
[3] Harvard Univ, Black Hole Initiat, 20 Garden St, Cambridge, MA 02138 USA
[4] Harvard & Smithsonian, Ctr Astrophys, 60 Garden St, Cambridge, MA 02138 USA
[5] Georgia Inst Technol, Ctr Relativist Astrophys, Howey Phys Bldg, 837 State St NW, Atlanta, GA 30332 USA
[6] Harvard Univ, Inst Theory & Computat, 60 Garden St, Cambridge, MA 02138 USA
[7] Flatiron Inst, Ctr Computat Astrophys, New York, NY 10010 USA
[8] Columbia Univ, Dept Phys, Pupin Hall, New York, NY 10027 USA
[9] Columbia Univ, Columbia Astrophys Lab, Pupin Hall, New York, NY 10027 USA
基金
美国国家科学基金会;
关键词
M87 EVENT HORIZON; MAGNETICALLY ARRESTED ACCRETION; HIGH-ENERGY NEUTRINOS; GRMHD SIMULATIONS; RADIATIVE EFFICIENCY; 3C; 84; SCALE; PROPAGATION; AGN; ACCELERATION;
D O I
10.3847/2041-8213/ad24fc
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Accreting supermassive black holes (SMBHs) produce highly magnetized relativistic jets that tend to collimate gradually as they propagate outward. However, recent radio interferometric observations of the 3C 84 galaxy reveal a stunning, cylindrical jet already at several hundred SMBH gravitational radii, r greater than or similar to 350r g. We explore how such extreme collimation emerges via a suite of 3D general relativistic magnetohydrodynamic simulations. We consider an SMBH surrounded by a magnetized torus immersed in a constant-density ambient medium that starts at the edge of the SMBH sphere of influence, chosen to be much larger than the SMBH gravitational radius, r B = 103 r g. We find that radiatively inefficient accretion flows (e.g., M87) produce winds that collimate the jets into parabolas near the black hole. After the disk winds stop collimating the jets at r less than or similar to r B, they turn conical. Once outside r B, the jets run into the ambient medium and form backflows that collimate the jets into cylinders some distance beyond r B. Interestingly, for radiatively efficient accretion, as in 3C 84, the radiative cooling saps the energy out of the disk winds; at early times, they cannot efficiently collimate the jets, which skip the initial parabolic collimation stage, start out conical near the SMBH, and turn into cylinders already at r similar or equal to 300r g, as observed in 3C 84. Over time, the jet power remains approximately constant, whereas the mass accretion rate increases; the winds grow in strength and start to collimate the jets, which become quasi-parabolic near the base, and the transition point to a nearly cylindrical jet profile moves outward while remaining inside r B.
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页数:11
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