Toward First-Principle Simulations of Galaxy Formation: I. How Should We Choose Star-Formation Criteria in High-Resolution Simulations of Disk Galaxies?
Toward First-Principle Simulations of Galaxy Formation: I. How Should We Choose Star-Formation Criteria in High-Resolution Simulations of Disk Galaxies?
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走向星系形成的第一原理模拟:一、盘状星系高分辨率模拟中我们应该如何选择恒星形成标准?
DOI:
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发表时间:
2008
期刊:
影响因子:
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通讯作者:
N. Yoshida
中科院分区:
文献类型:
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作者:
Takayuki R.Saitoh;H. Daisaka;E. Kokubo;J. Makino;T. Okamoto;K. Tomisaka;K. Wada;N. Yoshida
We performed three-dimensional N -body/SPH simulations to study how mass resolution and other model param- eters, such as the star-formation efficiency parameter, Cand the threshold density for star formation, nth affect structures of the galactic gaseous/stellar disk. We employed 10 6 -10 7 particles to resolve a cold ( T 100 cm � 3 ) phase as well as diffuse, hot phases. We found that structures of the interstellar medium (ISM) and the distribution of young stars were sensitive to the assumed values of nth. High-nth models with nth = 100 cm � 3 yielded clumpy multi-phase features in the ISM. Young stars were distributed in a thin disk, of which the half-mass scale height was 10-30 pc. In low-nth models with nth = 0.1 cm � 3 , which is usually employed in cosmological galaxy-formation simulations, the gas disk appears to be smoother and the stellar disk is found to be several-times thicker than the high-nth models. A high-resolution simulation with high-nth is necessary to reproduce the complex structure of the gas disk. The global star-formation properties of galaxies, such as the star-formation history, in low-nth models are similar to those in high-nth models when we tune the value of Cso that they repro- duce the observed relation between the surface gas density and the surface star-formation rate density. We however emphasize that high-nth models automatically reproduce the relation, regardless of the values of C� .T he ISM structure, phase distribution and distributions of young star-forming regions are quite similar in runs with different values of C� . We found that the timescale of the flow from the reservoir (nH � 1c m � 3 ) to the star-forming regions (nH & 100cm � 3 ) is about five-times as long as the local dynamical time, and this evolution timescale is independent