Formation and evolution of primordial protostellar systems

被引:277
作者
Greif, Thomas H. [1 ]
Bromm, Volker [2 ,3 ]
Clark, Paul C. [4 ]
Glover, Simon C. O. [4 ]
Smith, Rowan J. [4 ]
Klessen, Ralf S. [4 ]
Yoshida, Naoki [5 ]
Springel, Volker [6 ,7 ]
机构
[1] Max Planck Inst Astrophys, D-85740 Garching, Germany
[2] Univ Texas Austin, Dept Astron, Austin, TX 78712 USA
[3] Univ Texas Austin, Texas Cosmol Ctr, Austin, TX 78712 USA
[4] Heidelberg Univ, Zentrum Astron, Inst Theoret Astrophys, D-69120 Heidelberg, Germany
[5] Univ Tokyo, Inst Phys & Math Universe, Kashiwa, Chiba 2778568, Japan
[6] Heidelberg Inst Theoret Studies, D-69118 Heidelberg, Germany
[7] Heidelberg Univ, Zentrum Astron, Astron Recheninst, D-69120 Heidelberg, Germany
基金
美国国家科学基金会; 日本学术振兴会;
关键词
hydrodynamics; stars: formation; galaxies: high-redshift; cosmology: theory; early Universe; INITIAL MASS FUNCTION; III STAR-FORMATION; 1ST STARS; MAGNETIC-FIELDS; SINK PARTICLES; HII REGION; SIMULATIONS; ACCRETION; STELLAR; GAS;
D O I
10.1111/j.1365-2966.2012.21212.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We investigate the formation of the first stars at the end of the cosmic dark ages with a suite of three-dimensional, moving-mesh simulations that directly resolve the collapse of the gas beyond the formation of the first protostar at the centre of a dark matter minihalo. The simulations cover more than 25 orders of magnitude in density and have a maximum spatial resolution of 0.05 R?, which extends well below the radius of individual protostars and captures their interaction with the surrounding gas. In analogy to previous studies that employed sink particles, we find that the Keplerian disc around the primary protostar fragments into a number of secondary protostars, which is facilitated by H2 collisional dissociation cooling and collision-induced emission. The further evolution of the protostellar system is characterized by strong gravitational torques that transfer angular momentum between the secondary protostars formed in the disc and the surrounding gas. This leads to the migration of about half of the secondary protostars to the centre of the cloud in a free-fall time, where they merge with the primary protostar and enhance its growth to about five times the mass of the second most massive protostar. By the same token, a fraction of the protostars obtain angular momentum from other protostars via N-body interactions and migrate to higher orbits. On average, only every third protostar survives until the end of the simulation. However, the number of protostars present at any given time increases monotonically, suggesting that the system will continue to grow beyond the limited period of time simulated here.
引用
收藏
页码:399 / 415
页数:17
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