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LOW-MASS STAR FORMATION TRIGGERED BY SUPERNOVAE IN PRIMORDIAL CLOUDS

机译:超新星在本源云中触发的低质量恒星形成

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The evolution of a gas shell, swept up by the supernova remnant of a massive first-generation star, is studied with H_2 and HD chemistry taken into account and with the use of a semianalytical approximation to the dynamics. When a first-generation star, formed in a parent pregalactic cloud, explodes as a supernova with explosion energy in the range of 10~(51)-10~(52) ergs at redshifts of z = 10-50, H_2 and HD molecules are formed in the swept up gas shell at fractional abundances of ~ 10~(-3) and ~10~(-5), respectively, and effectively cool the gas shell to temperatures of 32-154 K. If the supernova remnant can sweep to gather the ambient gas of mass 6 x 10~4 to 8 x 10~5 solar mass, the gas shell comes to be dominated by its self-gravity and, hence, is expected to fragment. The amount of swept up gas necessary for fragmentation increases with the explosion energy and decreases with the interstellar gas density (or redshift) of the host cloud, which provides a lower boundary to the mass of the host cloud in which star formation is triggered by the first-generation supernova. Also, the condition for fragmentation is very sensitive to the thermal state of interstellar gas. Our result shows that for a reasonable range of temperatures (200-1000 K) of interstellar gas, the formation of second-generation stars can be triggered by a single supernova or hypernova with explosion energy in the above range in a primordial cloud of total (dark and baryonic) mass as low as a few times 10~6 solar mass. For higher temperatures in the interstellar gas, however, the condition for the fragmentation in the swept up gas shell demands a larger supernova explosion energy. We also follow the subsequent contraction of the fragment pieces assuming their geometry (sphere and cylinder) and demonstrate that the Jeans masses in the fragments decrease to well below 1 solar mass by the time the fragments become optically thick to the H_2 and HD lines. The fragments are then expected to break up into dense cores whose masses are comparable to the Jeans masses and collapse to form low-mass stars that can survive to the present. If the material in the gas shell is mixed well with the ejecta of the supernova, the shell and low-mass stars thus formed are likely to have metals of abundance [Fe/H] approx= -3 on average. This metallicity is consistent with those of the extremely metal-poor stars found in the Galactic halo. Stars with low metallicities of [Fe/H] < -5 such as HE 0107-5240, recently discovered in the Galactic halo, are difficult to form by this mechanism and must be produced in different situations.
机译:研究了被大质量第一代恒星的超新星残留物扫掠的气壳的演化,并考虑了H_2和HD化学,并使用动力学的半解析近似法。当在母系前银河云中形成的第一代恒星以超新星爆炸时,其爆炸能量在z = 10-50,H_2和HD分子的红移范围内为10〜(51)-10〜(52)erg。在扫掠的气壳中分别以〜10〜(-3)和〜10〜(-5)的分数丰度形成,并有效地将气壳冷却至32-154 K的温度。如果超新星残余能扫过为了收集质量为6 x 10〜4到8 x 10〜5太阳质量的环境气体,气壳将由其自重控制,因此预计会破裂。碎裂所需的吹扫气体量随爆炸能量的增加而增加,并随宿主云的星际气体密度(或红移)而减少,这为宿主云的质量提供了一个较低的边界,在该边界中,恒星形成是由恒星形成触发的第一代超新星。同样,碎裂的条件对星际气体的热态非常敏感。我们的结果表明,对于星际气体的合理温度范围(200-1000 K),第二代恒星的形成可以由单个超新星或超新星触发,其爆炸能量在上述范围的总原始云中黑暗和重子)质量低至太阳质量的10〜6倍。但是,对于星际气体中较高的温度,扫掠的气体壳中碎片的条件需要更大的超新星爆炸能量。我们还假设了碎片的几何形状(球体和圆柱体),随后进行了收缩,并证明了当碎片对H_2和HD线的光学厚度增加时,碎片中的Jeans质量下降到远低于1太阳质量。然后,预计这些碎片会分裂成密度可与吉恩斯质量相提并论的致密核心,然后坍塌形成低质量的恒星,这些恒星可以生存到现在。如果气壳中的物质与超新星的喷出物充分混合,那么壳和如此形成的低质量恒星很可能平均具有[Fe / H]大约为-3的金属。这种金属性与银河晕中发现的极度贫金属的恒星一致。低金属度[Fe / H] <-5的恒星,例如最近在银河系光环中发现的HE 0107-5240,很难通过这种机制形成,必须在不同的情况下产生。

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